Patent Publication Number: US-10328357-B2

Title: DisClub Golf: disclub, golfdisc and discopter

Description:
RELATED APPLICATIONS 
     This is a Continuation in Part application claims priority of patent applications of U.S. patent application Ser. No. 15/472,262 filed Mar. 28, 2017, Ser. No. 14/541,152 filed Nov. 14, 2014 now U.S. Pat. No. 9,855,510 issued on Jan. 2, 2018, Ser. No. 13/918,989 filed Jun. 16, 2013, U.S. patent application Ser. No. 12/422,719 filed Apr. 13, 2009; U.S. patent application Ser. No. 12/317,973, filed Dec. 31, 2008, now U.S. Pat. No. 8,089,324 issued on Jan. 3, 2012; U.S. patent application Ser. No. 12/291,984, filed Nov. 12, 2008; U.S. patent application Ser. No. 12/291,618, filed Nov. 12, 2008, now U.S. Pat. No. 7,876,188 issued on Jan. 25, 2011; U.S. patent application Ser. No. 12/288,770, filed Oct. 23, 2008, now U.S. Pat. No. 7,663,349 issued on Feb. 16, 2010; U.S. patent application Ser. No. 12/229,412, filed Aug. 23, 2008, now U.S. Pat. No. 8,089,323 issued on Jan. 3, 2012; U.S. patent application Ser. No. 12/157,785, filed Jun. 14, 2008, now U.S. Pat. No. 7,857,718 issued on Dec. 28, 2010; U.S. patent application Ser. No. 12/074,143, filed Feb. 29, 2008, now U.S. Pat. No. 7,794,341 issued on Sep. 14, 2010; U.S. patent application Ser. No. 11/210,306, filed Aug. 24, 2005, now U.S. Pat. No. 7,422,531 issued on Sep. 9, 2008; U.S. patent application Ser. No. 10/842,739, filed May 10, 2004, now U.S. Pat. No. 7,101,293 issued on Sep. 5, 2006; U.S. patent application Ser. No. 09/127,255, Jul. 31, 1998, now U.S. Pat. No. 6,193,620 issued on Feb. 27, 2001; U.S. patent application Ser. No. 12/082,601, filed Apr. 12, 2008; U.S. patent application Ser. No. 12/079,179, filed Mar. 25, 2008, now U.S. Pat. No. 8,089,353 issued on Jan. 3, 2012; U.S. patent application Ser. No. 11/593,271, filed Nov. 6, 2006, now U.S. Pat. No. 7,511,589; U.S. patent application Ser. No. 11/500,125, filed Aug. 5, 2006, now U.S. Pat. No. 7,525,392 issued on Apr. 28, 2009; U.S. patent application Ser. No. 892,358, filed Jul. 14, 1997, now U.S. Pat. No. 5,850,093; U.S. patent application Ser. No. 854,800, filed Mar. 23, 1992, now U.S. Pat. No. 5,280,200; U.S. patent application Ser. No. 81,074, filed Jun. 22, 1993, now U.S. Pat. No. 5,793,125; U.S. patent application Ser. No. 577,792, filed Sep. 5, 1990, now U.S. Pat. No. 5,198,691; U.S. patent application Ser. No. 577,791, filed Sep. 5, 1990, now U.S. Pat. No. 5,111,076; which herein incorporated by reference in its entirety. 
    
    
     FIELD OF THE INVENTION 
     SAVE GOLF COURSE with DisClub Golf: Golf does not die, Long Live the Golf! 
     The conventional golf sport is the ball golf. The ball of golf sport is named as golf ball. To play the ball golf sport, Ball Golf is to use the two hands to swivel the club to have the snap hit on the golf ball to fly. 
     The conventional disc golf sport is the disc golf. To play the disc golf sport, disc golf is to use the single hand to swivel the hand to have the snap force to throw the disc to fly. 
     The DisClub Golf is a new golf sport invented by the Tarng Family. The disc of DisClub Golf is named as golfdisc. To play the disc golf sport, the disclub golf is to use the two hands to swivel the disclub to have the snap force to launch the golfdisc to fly. 
     Furthermore, to search the golfdisc in the golf course, the disclub golfer can use the discopter to search the lost golfdisc in the discgolf course. The discopter is headwear on the head of disclub golfer. The discopter can take off from the head of disc golfer. With the smart phone and video camera carried by the discopter, the disclub golfer can identify the lost golfdisc in the golf course or discgolf course. 
     All the golf sports, golf ball, disc golf and disclub golf, have something in common such as snap action. However, the disclub golf has many unique properties. There are many wrong concepts about disclub golf. 
     The snapping force in the golf sport is very important concept. At the instant of the launching time, there is the snapping action of suddenly applying the impulse force. The ball golf is to hit the still ball with the club head. It has the natural snapping force in the ball golf. 
     In the disc golf, as the hand swivels, the disc moves along with the hand to build the disc momentum. The hand grasps the disc firmly. However, the disc is already moving in the swivel of hand. At the launching point of disc, the golfer suddenly applies the impulse force to the disc with the snapping action. The snapping action of hand is made along the tangent direction of the disc trajectory. Due to the firm grasp of hand, all the snapping impulse momentum is transmitted to the disc to be the disc flying momentum efficiently. 
     Similarly, to have the snapping throw of the golfdisc, the golfdisc cannot dangle freely on the disclub head. In the disclub golf sport, to transfer the energy from the disclub to the golfdisc efficiently, the disclub head has to grasp the golfdisc firmly. The cam locking is adopted to hold the golfdisc to the disclub head to transfer the snapping impulse momentum from the disclub to golfdisc efficiently. 
     The disc has the best performance is to have the same profile in all the directions. The disc of conventional disc golf is perfect symmetry to have the best performance. The golfdisc of the disclub golf is different from the disc of disc golf. The modifications of the conventional disc with the addition of discap to be the golfdisc will deteriorate the disc flying performance. Therefore, it is to modify the disc of disc golf to be the golfdisc of disclub golf with the minimum disturbance of the airflow. The following principles must be followed to modify golfdisc to keep the best performance of the original disc of disc golf. 
     The principles to modify disc and the rule of thumbs of the golfdisc design are as follows.
         (1) All the discap of the golfdisc is embedded in the disc.   (2) The size of the discap opening is minimized.   (3) To minimize the cap opening,
           The middle portion of the discap is filled up with whistle type plateau.   
           (4) (A) The disc takes off the disclub head is in the horizontal direction with the slicing action that the bottom plate is flat and horizontal.
           (B) To minimize the effect of discap, the air does not blow into the discap.
               The bottom edge is 0 degree that the air will not blow into the discap.   The bottom edge serves as the horizontal stabilizer.   
               
           (5) At the front edge, the trail flap is a triangle to increase the lift.
           At the right and left edges, the trail flap serves as the vertical stabilizer.   At the rear edge, the trail flap reduces the air injecting into the cavity of discap to reduce the drag.   
               

     Many thanks to Mrs. Shun-Yu Nieh and Jwu-Ing Tarng, the King of Golf is back. It is the disclub golf saving both the golf and the golf course. Even for the previous old version of disclub golf, there are already many people expressing to buy the disclub golf. However, we hold it until we have made the technology breakthrough of cam locking and Super-Drift Tangs-Force golfdisc as disclosed in this patent application. For the popular convenience, the people who are interested to buy the cutting-edge dual phone DP, discopter, golfdisc and disclub of disclub golf, please contact Dr. Min Ming Tang as follows: Nobleman Son School, Golf/DisClub Golf Kid School, Kedi Art School/Kids of Jedi School, and Zedi Art School/the Last Jedi School, PDCGA, TANG SYSTEM, 4225 Borina Drive, San Jose, Calif. 95129, Tel: (408)-446-3163; (408)-504-7530(Cellular), Email: pdcfga@gmail.com, tangsystem@gmail.com; the official Profession DisClub Golf Association PDCGA Website: http://www.PDCFGA.com. The Kedi is the Kid of Jedi. The Kedi Art School teaches the versatile modern Jedi arts including the DisClub Golf of DisClub and GolFrisbee. 
     Long Live the Golf ! Golf does not die, Golf just becomes the next generation DisClub Golf. Ball Golf is dying. Even though the Disc Golf is rising, however, due to the Disc Golf requirement of body strength, the Disc Golf cannot be the next generation Golf, either. The only hope is the DisClub Golf which is the hybrid of Ball Golf and Disc Golf. 
     DisClub Golf—the Greatest Innovation in Golf and Disc Golf: (1) Enjoy Disc Golf w/o the requirements of strong body; (2) Bring the kids, ladies, wife and grandparents together to enjoy healthy Family Golf sport; (3) it might SAVE GOLF COURSE with DisClub Golf. The Professional DisClub Golf Association (PDCGA) head quarter is located at 4225 Borina Drive, San Jose, Calif. 95129. PDCGA not only has the DisClub Golf Proshop selling the DisClub and GolFrisbee but also “ZeDi Camp: NxGen Kids Golf School/Class” provides three classes in series:
         (1) Noble/Nobleman Son/Kid School( );   (2) Golf/Golfman Son/Kid School( ) (Kedi Art School/Kids of Jedi School);   (3) Zedi/Zediman Son/Kid School ( ) (Zedi Art School/the Last Jedi School).
 
The Nobleman Son School is to train the whole body Snap force capability and the Nobleman Son academic Sage studies of the greatest Oriental Emperor&#39;s knowledge and Performance. The Golfman Son School is to train the DisClub Snap force capability and the ball and disc air dynamic academic studies. Zediman Son School is to train the last Jedi the supernatural and inter-star mental communication capability for the star war of Zediman Son.
       

     The FaceBook Group of PDCGA:Professional DisClub Golf Association is
         https://www.facebook.com/groups/217281025597009/       

     The Snap is the most important factor in the Long Drive of DisClub Golf. The Grand Demo of DisClub Golf is posted on the Youtube,
         https://www.youtube.com/watch?v=W_mJrLPDMfk       

     The Grand Demo of DisClub Golf: 
     (1) the Long Drive Demo with the “Prototype” of Disclub Golf made of “Fishing Pole”; 
     (2) the Putt Demo with the GolFrisbee and Golf Club of the 2nd Generation DisClub Golf; and 
     (3) the Grand Demo with the 1st Generation GolfRing. 
     For the safety purposes, in this Grand Demo, the Golf Ring was thrown into the cloud like the arrow did. Due to the swivel to fly with the club, the golfring flied so fast that you hardly saw it until it fell downward. In the future, for the coming the 4th Generation DisClub sample, the club of the DisClub Golf will be made of the Golf Club and swivel as the Golf does. 
     BACKGROUND FIELD OF INVENTION 
     The disclub golf is the disc golf for the old retired man. The old retired man stands still and swivels the disclub to launch the disc. It is similar to the traditional ball golf. With the flagpole being replaced by the inverted umbrella type flagpole, the disclub golf can play on the golf course, too. 
     Disclub golf is the new golf sport invented by the Tarng Family. It is dedicated for the old retired men who liked the disc golf as they were young. However, as the disc golfers become old, they are no more able to play the disc golf in the rough disc golf course. The old disc golfer can play the disclub golf in the plain golf course. The disclub golf is compatible with the ball golf to play in the same golf course. 
     The golf ball can be hit with the launching angle to be 45° relative the ground. The 45° is to have the maximum throwing distance for golf ball. However, the conventional disc is thrown with 0° relative to the ground. 
     Furthermore, on the golf ball, there are dimples to enhance the golf ball flying distance. The golf ball dimples use the Magnus force to enhance the flying distance. However, in the conventional disc, the surface of disc is flat. There are no dimples on disc surface to enhance the distance. 
     On our invention Tarng golfdisc, there are dimples on the surface of disc. With the dimples, the Tarng Force can increase the launch angle from 0° to 45°, etc. With the increment of the launching angle from 0° to 45°, the dimples on the Tarng golfdisc surface can enhance the flying distance of the Tarng disc. 
     For the single piece aerofoil, the subsonic aerofoil has the round head. The supersonic aerofoil has the sharp triangle. The conventional disc is in subsonic operation range. However, the edge of the bottom edge of golfdisc is in the sharp triangle shape. 
     Furthermore, for the two-piece aerofoil, there is a flap at the tail edge of the aerofoil. To increase the lift force, the flap rotates downward. 
     The super-lift Tang golfdisc combines the above characteristics to be unique high lift disc. The golfdisc has the right triangle rim. The bottom edge of the rim is horizontal. The tail edge of the bottom edge has a triangle flap. At the front rim of the disc, the triangle flap servers as the downward flap to increase the lift. At the side rim of the disc, the triangle serves as the stability fin. At the rear rim of the disc, the triangle flap reduces the air blowing into the bore of the discap to reduce the drag. The super-lift Tang golfdisc can increase the drift capability and the gliding distance of the disc. 
     The super-lift Tang golfdisc of the disclub golf is different from the conventional disc of disc golf. As the super-lift Tang golfdisc launches from the disclub head, it is in the horizontal slicing action. The horizontal bottom plane can increase the horizontal operation angle of the launching disc. Furthermore, the horizontal bottom plane can reduce the air blowing into the bore to reduce the drag force of golfdisc. 
     The disc golf course usually locates in the rugged terrain. To make it easy to carry the disclub, the telescopic disclub is adopted. The telescopic disclub uses the screws to adjust and fix the length of disclub. Due to the swivel of the disclub, the reaction force of the disc will twist the telescopic disclub. The screw must be self-tighten due to the twist of the telescopic disclub. Therefore, there are the right-hand telescopic disclub and left-hand telescopic disclub. 
     The headwear discopter is to search the lost golfdisc in the golf course or discgolf course. There is a smart phone and video camera carried by the discopter. The headwear discopter takes off from the head of the disc golfer and searches the lost golfdisc in the golf course. The video is transmitted from the smart phone and video camera and transmitted back to the wrist-wear monitor for the disclub golfer to identify the lost golfdisc. 
     BACKGROUND-DESCRIPTION OF PRIOR ART 
     The ball golf is dead. It is declared by Lisa Gray, the Gray Matters Columnist, Houston Chronicle.
         http://www.houstonchronicle.com/local/gray-matters/article/Golf-is-dead-5589999.php       

     In the following article,
         Golfs/Disc Golf Decline: 5 Reason Why Golf/Disc Golf are Dying Sport|Money—Time       

     Jun. 13, 2014−“While other sports have embraced new technology and innovation with open arms, traditionalists strive to protect the game of golf and keep them exactly as they love them-even in the face of suffering courses and shrinking audiences.”
         http://www.time.com/money/2871511/golf-dying-tiger-woods-elitist/       

     The disc golf is going to replace the ball golf. The conventional disc is hand thrown disc. It uses the hand to grasp the disc to swivel the disc to build up the momentum to maintain the flying direction and stability. As the disc is launched to fly, the hand uses the snapping action to apply the impulse force to the disc. 
     However, the ball golf is for the old retired man. The disc golf is for the young sportsman. They are two different segments of the sporting population. There is no disc golf for the old retired man. The conventional disc golf needs to run and throw the disc as the diskette does. The old retired man is too old to play the conventional disc golf. 
     All the conventional disc is thrown horizontally. It cannot use the increment of the launch angle to increase the disc flying distance. Furthermore, the conventional disc does not have the dimples to increase the flying distance. 
     There is no disclub golf before. There is no disclub to throw the disc. There is no disclub having the capability to apply the snapping force to launch the disc to fly. For the conventional disc, there is no disc having the super-lift at the low speed to increase the drift and gliding distance. 
     DisClub Golf is allowed to use both Disclub and hand to throw the disc. However, to avoid the snap causing the disc golf sporting injuries, for more than 400 feet throw, it strongly suggests to use the disclub as the “golf wood club” to throw disc. Disc Golf uses the arm as the Golf wood club. The golfer can change the broken wood club with the new Golf wood club. However, the disc golfer cannot change his wound arm with a new arm. 
     As shown in the following medical reports in journals, 
     Jun. 25, 2015 Disc Golf, a Growing Sport: Description and Epidemiology of Injuries . . . .
         http://journals.sagepub.com/doi/full/10.1177/2325967115589076
 
Disc golf is a sport played much like traditional golf, but rather than using a ball and club, players throw flying discs with various throwing motions. It has been played by an estimated 8 to 12 million people in the United States. Like all sports, injuries sustained while playing disc golf are not uncommon. Although formalized in the 1970s, it has grown at a rapid pace; however, disc golf-related injuries have yet to be described in the medical literature. More than 81% of respondents stated that they had sustained an injury playing disc golf, including injuries to the elbow (n=325), shoulder (n=305), back (n=218), and knee (n=199). The injuries were most commonly described as a muscle strain (n=241), sprain (n=162), and tendinitis (n=145).
       

     Objects and Advantages 
     To have the long distance drive, the snapping action is needed. The cam locking enables the snapping action of the disclub to apply the impulse force on the golfdisc. The dimples on the Tarng disc surface can increase the launch angle to enhance the flying distance to the disc. To enhance the flying distance, the super-lift disc has the flat bottom with the triangle flap to increase the drift and gliding distance of the golfdisc. The telescopic disclub is easy to carry in the rugged terrain. The head-wearing golfdisc or discopter can serve as the hat. The head-wearing discopter has the smart phone and camera, etc. to transmit the video signal to the wrist-wear monitor. Having the joints, with the smart phone and video camera, the golfdisc mounting on telescopic disclub serves as the self-portrait camera. 
    
    
     
       DRAWING FIGURES 
       FIG.  1 A 1  is the raising position to start the swivel of the basic disclub; FIG.  1 A 2  is the disclub at the snapping position of the swivel; FIG.  1 A 3  is the golfdisc at the launching position being ready to fly; FIG.  1 A 4  is the golfdisc taking off to fly in the sky; FIG.  1 B 1  is the raising position to start the swivel of the golf-club style disclub; FIG.  1 B 2  is the golf-club style disclub at the snapping position; FIG.  1 B 3  is the golfdisc at the launching position of the golf-club style disclub being ready to fly; FIG.  1 B 4  is the golfdisc of the golf-club style disclub taking off to fly in the sky; FIG.  1 C 1  is the telescopic disclub in the elongation position; FIG.  1 C 2  is the telescopic disclub in the shortened position; FIG.  1 C 3  is the extendable disclub in the extended position; FIG.  1 C 4  is the extendable disclub in the shortened position; FIG.  1 C 5  is the top view of the DisClub in the extendable disclub in the extended position; FIG.  1 C 6  is the top view of the DisClub in the extendable disclub in the shortened position; FIG.  1 C 7  is the side view of the DisClub in the extendable disclub in the extended position; FIG.  1 C 8  is the side view of the DisClub in the extendable disclub in the shortened position; FIG.  1 D 1  is the adjustable angle golf-club style disclub launching the disc to fly; it shows the DisClubGolfdisc combining with DisGolf; FIG.  1 D 2 A is the adjustable angle golf-club style disclub at the launching position; swiveling the club to throw the golf ring on the flag pole as the quoits does; FIG.  1 D 2 B is the adjustable angle golf-club style disclub in the folded position; FIG.  1 E 1  is the telescopic disclub at the self-portrait position; FIG.  1 E 2  is the telescopic disclub in the normal discgolf operation. They are the operations of the basic disclub golf, golf-club style disclub golf, telescopic disclub and golf-club style telescopic disclub. 
         FIG. 2A  is the trajectories of the golf ball;  FIG. 2B   1  is velocity profiles of the golf ball; FIG.  2 B 2  is the Magnus force applied to the analysis of the velocity profiles of the golf ball. 
         FIG. 3A  is the disc attitudes varying along the flying velocity; FIG.  3 B 1  is the disc attitudes varying along the flying path; FIG.  3 B 2  is the disc attitudes having the Tarng force varying along the flying path. 
       FIG.  4 A 1  is the isometric top view of the super-lift golfdisc; FIG.  4 A 2  is the transparent solar cell version of the isometric top view of the super-lift golfdisc;  FIG. 4B   1  is the top view of the super-lift golfdisc; FIG.  4 B 2  is the transparent solar cell version of the top view of the super-lift golfdisc; FIG.  4 C 1  is the isometric bottom view of the super-lift golfdisc; FIG.  4 C 2  is the transparent solar cell version of the isometric bottom view of the super-lift golfdisc;  FIG. 4D  is the side view of the super-lift golfdisc;  FIG. 4E  is the transparent solar cell version of the side view of the super-lift golfdisc;  FIG. 4F  is the section version of the side view of the super-lift golfdisc. 
       FIG.  5 A 1  is the dynamic analysis of the disc in the high speed air flow with the center of pressure being located at the rear of the center of gravity in the counter-clockwise rotation of disc; FIG.  5 A 2  is the dynamic analysis of the disc in the high speed air flow with the center of pressure being located at the front of the center of gravity in the counter-clockwise rotation of disc; FIG.  5 B 1  is the dynamic analysis of the disc in the high speed air flow with the center of pressure being located at the rear of the center of gravity in the clockwise rotation of disc; FIG.  5 B 2  is the dynamic analysis of the disc in the high speed air flow with the center of pressure being located at the front of the center of gravity in the clockwise rotation of disc;  FIG. 5C  is the trajectory of the flying disc; FIG.  5 C 1  is the dynamic analysis of the disc in the high speed air flow with the center of pressure being located at the rear of the center of gravity in the clockwise rotation of disc as shown in  FIG. 5C ; FIG.  5 C 2  is the dynamic analysis of the disc in the high speed air flow with the center of pressure being located at the front of the center of gravity in the clockwise rotation of disc as shown in  FIG. 5C . 
       FIG.  6 A 1  is the isometric top view of the super-lift Tarng golfdisc having the Tarng force; FIG.  6 A 2  is the transparent version of the isometric top view of the super-lift Tarng golfdisc having the Tarng force; FIG.  6 B 1  is the isometric bottom view of the super-lift Tarng golfdisc having the Tarng force; FIG.  6 B 2  is the transparent version of the isometric bottom view of the super-lift Tarng golfdisc having the Tarng force; FIG.  6 C 1  is the transparent version of the side view of the super-lift Tarng golfdisc having the Tarng force; FIG.  6 C 2  is the transparent version of the section view of the super-lift Tarng golfdisc having the Tarng force to be implemented with the concave dimples; FIG.  6 C 3  is the transparent version of the section view of the super-lift Tarng golfdisc having the Tarng force to be implemented with the convex dimples. 
       FIG.  7 A 1  is the golfdisc having the Tarng force in the counter-clockwise rotation; FIG.  7 A 2  is the dynamic analysis of the golfdisc for the Tarng force in the counter-clockwise rotation;  FIG. 7B   1  is the golfdisc having the Tarng force in the clockwise rotation; FIG.  7 B 2  is the dynamic analysis of the golfdisc for the Tarng force in the clockwise rotation; 
       FIG.  8 A 1  is the dynamic analysis for the golfdisc having the Tarng force rotating in the counter-clockwise direction having the center of pressure CP located after the center of gravity CG; FIG.  8 A 2  is the dynamic analysis for the golfdisc having the Tarng force rotating in the counter-clockwise direction having the center of pressure CP located before the center of gravity CG; FIG.  8 B 1  is the dynamic analysis for the golfdisc having the Tarng force rotating in the clockwise direction having the center of pressure CP located after the center of gravity CG; FIG.  8 B 2  is the dynamic analysis for the golfdisc having the Tarng force rotating in the clockwise direction having the center of pressure CP located before the center of gravity CG. 
         FIG. 9A  is the side view of the flying trajectory and attitudes of the Tarng golfdisc having the Tarng force;  FIG. 9B  is the front view of the flying trajectory and attitudes of the Tarng golfdisc having the Tarng force;  FIG. 9C  is the dynamic analysis of the Tarng golfdisc having the Tarng force. 
       FIG.  10 A 1  is the isometric top view of the super-lift Tarng golfdisc having the Tarng force on top side and bottom side; FIG.  10 A 2  is the transparent version of the isometric top view of the super-lift Tarng golfdisc having the Tarng force on both top side and bottom side; FIG.  10 B 1  is the isometric bottom view of the super-lift Tarng golfdisc having the Tarng force on both top side and bottom side; FIG.  10 B 2  is the transparent version of the isometric bottom view of the super-lift Tarng golfdisc having the Tarng force on both top side and bottom side. 
         FIG. 11A  is the transparent version of the top view of the super-lift Tarng golfdisc having the Tarng force on both top side and bottom side;  FIG. 11B  is the section view along the center line CL L -CL L  for the super-lift Tarng golfdisc having the Tarng force to be implemented with the concave dimples having the Tarng force on both top side and bottom side;  FIG. 11C  is the section view along the center line CL R -CL R  for the super-lift Tarng disc having the Tarng force to be implemented with the concave dimples on both top side and bottom side. 
       FIG.  12 A 1  is the isometric top view of the super-lift Tarng golfdisc having the rim adaptor, FIG.  12 A 2  is the transparent version of isometric top view of the super-lift Tarng golfdisc having the rim adaptor; FIG.  12 B 1  is the isometric bottom view of the super-lift Tarng golfdisc having the rim adaptor; FIG.  12 B 2  is the transparent version of isometric bottom view of the super-lift Tarng golfdisc having the rim adaptor;  FIG. 12C  is the section view of the super-lift Tarng golfdisc having the rim adaptor. 
         FIG. 13A  is the top view of the discopter super-lift Tarng golfdisc having the rim adaptor;  FIG. 13B  is the bottom view of the discopter super-lift Tarng golfdisc having the rim adaptor;  FIG. 13C  is the side view of the discopter super-lift Tarng golfdisc having the rim adaptor. 
       FIG.  14 A 1  is the isometric top view of the discopter; FIG.  14 A 2  is the transparent version of the isometric top view of the discopter;  FIG. 14B   1  is the isometric bottom view of the discopter; FIG.  14 B 2  is the transparent version of the isometric bottom view of the discopter. 
       FIG.  15 A 1  is the isometric top view of the discopter having the smart phone and microphone; FIG.  15 A 2  is the solar cell version of the isometric top view of the discopter having the smart phone and microphone; FIG.  15 B 1  is the isometric bottom view of the discopter having the smart phone and microphone; FIG.  15 B 2  is the solar cell version of the isometric bottom view of the discopter having the smart phone and microphone. 
       FIG.  16 A 1  is the isometric top view of the discopter in the disc-ring shape having the smart phone and microphone; FIG.  16 A 2  is the solar cell version of the isometric top view of the discopter in the disc-ring shape having the smart phone and microphone;  FIG. 16B   1  is the isometric bottom view of the discopter in the disc-ring shape having the smart phone and microphone; FIG.  16 B 2  is the solar cell version of the isometric bottom view of the discopter in the disc-ring shape having the smart phone and microphone; FIG.  16 C 1  is the section view of the discopter in the disc-ring shape having the smart phone and microphone; FIG.  16 C 2  is the section view of the discopter in the disc-ring shape having the propellers; FIG.  16 C 3  is the top isotropic view to show the discopter serving as for the Head Wearing Device of the Smart Hat of iHat; FIG.  16 C 4  is the front view to show the discopter serving as for the Head Wearing Device of the Smart Hat of iHat. 
       FIG.  17 A 1  is the isometric top view of the discopter in the disc-ring shape having the adjustable rim for the different size of the head; FIG.  17 A 2  is the solar cell version of the isometric top view of the discopter in the disc-ring shape having the adjustable rim for the different size of the head; FIG.  17 B 1  is the isometric bottom view of the discopter in the disc-ring shape having the adjustable rim for the different size of the head; FIG.  17 B 2  is the solar cell version of the isometric bottom view of the discopter in the disc-ring shape having the adjustable rim for the different size of the head; FIG.  17 C 1  is the side view of the thick golfring; FIG.  17 C 2  is the section isotropic view of the thick golfring; FIG.  17 C 3  is the bottom isotropic view of the thick golfring; FIG.  17 D 1  is the side view of the thin golfring; FIG.  17 D 2  is the section isotropic view of the thin golfring; FIG.  17 D 3  is the bottom isotropic view of the thin golfring. 
       FIG.  18 A 1  is the isometric top view of the discopter in the disc shape having the adjustable rim for the different size of the head; FIG.  18 A 2  is the solar cell version of the isometric top view of the discopter in the disc shape having the adjustable rim for the different size of the head;  FIG. 18B   1  is the isometric bottom view of the discopter in the disc shape having the adjustable rim for the different size of the head; FIG.  18 B 2  is the solar cell version of the isometric bottom view of the discopter in the disc shape having the smart phone. 
       FIG.  19 A 1  is the isometric top view of the discopter in the flexible hat shape having the adjustable rim for the different size of the head; FIG.  19 A 2  is the solar cell version of the isometric top view of the discopter in the flexible hat shape having the adjustable rim for the different size of the head; FIG.  19 B 1  is the isometric bottom view of the discopter in the flexible hat shape having the adjustable rim for the different size of the head; FIG.  19 B 2  is the solar cell version of the isometric bottom view of the discopter in the flexible hat shape having the smart phone. 
         FIG. 20A  is the side view of the super-lift disc to show the golfdisc profile of the disclub golf;  FIG. 20B  is the transparent version of the side view of the super-lift golfdisc to show the discap structure and the golfdisc profile of the disclub golf;  FIG. 20C  is the section view of the super-lift golfdisc to show the discap structure and the golfdisc profile of the disclub golf. 
         FIG. 21A  is the side view of the super-lift Tarng golfdisc to show the golfdisc profile of the disclub golf;  FIG. 21B  is the section view of the super-lift Tarng golfdisc to show the discap structure and the golfdisc profile of the disclub golf having low air drag force; FIG.  21 C 1  is the enlarged section view of the super-lift Tarng golfdisc to show the discap structure and the golfdisc profile of the disclub golf having the low air drag force; FIG.  21 C 2  is the enlarged section view of the super-lift Tarng golfdisc to show the golfdisc profile of the disclub golf having the low air drag force. 
         FIG. 22A  is the side view of the super-lift Tarng golfdisc to show the golfdisc having the subsonic aerofoil with flat bottom profile of the disclub golf;  FIG. 22B  is the transparent version of the side view of the super-lift Tarng golfdisc having the subsonic aerofoil with flat bottom to show the discap structure and the golfdisc profile of the disclub golf having the adaptable rim;  FIG. 22C  is the section view of the super-lift Tarng golfdisc having the subsonic aerofoil with flat bottom to show the discap structure and the golfdisc profile of the disclub golf having the adaptable rim;  FIG. 22D  is the bottom view of the super-lift Tarng golfdisc having the subsonic aerofoil with concave bottom to show the discap structure and the golfdisc profile of the disclub golf having the adaptable rim;  FIG. 22E  is the section view of the super-lift Tarng golfdisc having the subsonic aerofoil with concave bottom to show the discap structure and the golfdisc profile of the disclub golf having the adaptable rim;  FIG. 22F  is the section view of the rim for the super-lift Tarng golfdisc having the subsonic aerofoil with concave bottom to show the discap structure and the golfdisc profile of the disclub golf having the adaptable rim;  FIG. 22G  is the section view of the adaptor embedded in the rim for the super-lift Tarng golfdisc having the subsonic aerofoil with concave bottom to show the discap structure and the golfdisc profile of the disclub golf having the adaptable rim;  FIG. 22H  is the bottom view of the adaptor embedded in the rim for the super-lift Tarng golfdisc having the subsonic aerofoil with concave bottom to show the discap structure and the golfdisc profile of the disclub golf having the adaptable rim;  FIG. 22I  is the side transparent view of the DisClub Head for the super-lift Tarng golfdisc having the subsonic aerofoil with concave bottom to show the discap structure and the golfdisc profile of the disclub golf having the adaptable rim;  FIG. 22J  the flap and slat structure of the golfrisbee;  FIG. 22K  is the alternative view of the wing-fin-flap and slat structure of the golfrisbee;  FIG. 22L  is the bottom view of the wing-fin-flap and slat structure of the golfrisbee;  FIG. 22M  is the isotropic view of the wing-fin-flap and slat structure of the golfrisbee,  FIG. 22N  is the top view of the wing-fin-flap and bumper-fin-slat structure of the golfrisbee;  FIG. 22O  is the top view of the wing-fin-flap and bumper-fin-slat structure of the golfrisbee;  FIG. 22P  is the top view of the wing-fin-flap and bumper-fin-slat structure of the golfrisbee;  FIG. 22Q  is the injection module of the golfrisbee. 
         FIG. 23A  is the isometric section view of the discopter to show the discap structure;  FIG. 23B  is the isometric section view of the discopter to show the smart phone structure;  FIG. 23C  is the isometric section view of the discopter to show the propeller structure. 
         FIG. 24A  is the cam locking clip mechanism in the lock position;  FIG. 24B  is the force analysis of the cam locking clip mechanism. 
         FIG. 25A  is the bottom view of discap having the single cam locking clip mechanism;  FIG. 25B  is the isometric bottom view of discap having single cam locking clip mechanism;  FIG. 25C  is the isometric top view of discap having three anti-thrust poles. 
         FIG. 26A  is the top view of the disclub head having single cam locking clip mechanism;  FIG. 26B  is the isometric top view of the disclub head having the single cam locking clip mechanism;  FIG. 26C  is the isometric bottom view of the disclub head having the single cam locking clip mechanism; FIG.  26 D 1  is the disclub head of the extendable disclub; FIG.  26 D 2  is the transparent view of the disclub head for the extendable disclub. 
         FIG. 27A  is the top transparent view of the single cam locking clip mechanism in the lock position;  FIG. 27B  is the top transparent view of the single cam locking clip mechanism in the release position. 
       FIG.  28 A 1  is the bottom view of discap having the triple cam locking clip mechanism; FIG.  28 A 2  is the top view of disclub head having the triple cam locking clip mechanism; FIG.  28 B 1  is the isometric bottom view of discap having the triple cam locking clip mechanism; FIG.  28 B 2  is the isometric top view of disclub head having the triple cam locking clip mechanism. 
         FIG. 29A  is the top view of the triple cam locking clip mechanism in the release position;  FIG. 29B  is the top view of the triple cam locking clip mechanism in the first lock position;  FIG. 29C  is the top view of the triple cam locking clip mechanism in the second lock position;  FIG. 29D  is the top view of the triple cam locking clip mechanism in the third lock position; FIG.  29 E 1  shows the discap embedded in the golfrisbee; FIG.  29 E 2  shows the cave of the discap embedded in the golfrisbee after the discap being removed for the discap as shown in FIG.  29 E 5 ; FIG.  29 E 3  shows the bottom view of the discap; FIG.  29 E 4  shows the top view of the discap having the anti-shock stubs; FIG.  29 E 5  shows the top view of the discap having the concave structure for the plastic injection to reduce the shrinkage; FIG.  29 F 1  shows the adaptable discap embedded in the golfrisbee; FIG.  29 F 2  shows the bottom view of the adaptable discap; FIG.  29 F 3  shows the top view of the adaptable discap having the anti-shock stubs; FIG.  29 F 4  shows the cave of the adaptable discap embedded in the golfrisbee after the adaptable discap being removed for the discap as shown in FIG.  29 F 3 ; FIG.  29 F 5  shows the top view of the adaptable discap having the concave structure for the plastic injection to reduce the shrinkage; FIG.  29 F 6  shows the cave of the adaptable discap embedded in the golfrisbee after the adaptable discap being removed for the discap as shown in FIG.  29 F 5 ; FIG.  29 G 1  shows the foil stamping of golfrisbee; FIG.  29 G 2  shows the foil stamping of golfrisbee; FIG.  29 H 1  shows the foil stamping of golfrisbee; FIG.  29 H 2  shows the foil stamping of golfrisbee;  FIG. 29I  is the LOGO for Professional Woman DisClub Golf Association;  FIG. 29J  is the LOGO for DisClub Golf;  FIG. 29K  is the symbol of DisClub Golf. 
         FIG. 30A  is the isometric top view of the smart phone and video camera;  FIG. 30B  is the isometric bottom view of the smart phone and video camera. 
         FIG. 31A  is the isometric top view of the propeller and motor,  FIG. 31B  is the isometric bottom view of the propeller and motor. 
         FIG. 32A  is the right isometric view of the adjustable disclub head;  FIG. 32B  is the left isometric view of the adjustable disclub head;  FIG. 32C   1  is the bottom view of the adjustable disclub head; FIG.  32 C 2  is the bottom transparent view of the adjustable disclub head; FIG.  32 D 1  is the right isometric view of the rotatable head of the adjustable disclub head; FIG.  32 D 2  is the transparent version of the right isometric view of the rotatable head for the adjustable disclub head; FIG.  32 E 1  is the right isometric view of the adaptive fork of the adjustable disclub head; FIG.  32 E 2  is the transparent version of the right isometric view of the adaptive fork of the adjustable disclub head;  FIG. 32F  is the isometric view of the engaging plug for the adjustable disclub head. 
         FIG. 33A  is the isometric view of the basic disclub;  FIG. 33B  is the transparent version of the isometric view of the basic disclub;  FIG. 33C   1  is the extendable disclub in the extended position; FIG.  33 C 2  is the extendable disclub in the shortened position; FIG.  33 D 1  is the transparent view of the extendable disclub in the extended position; FIG.  33 D 2  is the transparent view of the extendable disclub in the shortened position. 
         FIG. 34A  is the isometric view of the golf-club style disclub;  FIG. 34B  is the transparent version of the isometric view of the golf-club style disclub. 
         FIG. 35A  is the golfdisc mounted on telescopic disclub in the elongation position having the callouts to show section views of disclub;  FIG. 35B  is the golfdisc mounted on the telescopic disclub in the shortened position having the callouts to show section views of disclub. 
       FIG.  36 A 1  is the isometric view of the telescopic disclub in the elongation position having the callouts to show section views of disclub; FIG.  36 A 2  is the transparent view of the isometric view of the telescopic disclub in the elongation position having the callouts to show section views of disclub; FIG.  36 A 3  is the isometric view of the torqueless telescopic disclub in the elongation position; — FIG. 36B   1  is the isometric view of the telescopic disclub in the shortened position having the callouts to show section views of disclub; FIG.  36 B 2  is the transparent view of the isometric view of the telescopic disclub in the shortened position having the callouts to show section views of disclub; FIG.  36 B 3  is the isometric view of the torqueless telescopic disclub in the shortened position. 
         FIG. 37A  is the locking screw design for the right hand throw telescopic disclub golf having the callouts to show section views of disclub;  FIG. 37B  is the locking screw design for the left hand throw telescopic disclub golf having the callouts to show section views of disclub;  FIG. 37C  is the transparent view of the extendable disclub in the extended position;  FIG. 37D  is the transparent view of the extendable disclub in the shortened position. 
       FIG.  38 A 1  is the right isometric view of the handle of the disclub; FIG.  38 A 2  is the left isometric view of the handle of the disclub; FIG.  38 B 1  is the exterior tube of the telescopic disclub having elliptical or non-circular section; FIG.  38 B 2  is the transparent view of the exterior tube of the telescopic disclub having circular section; FIG.  38 B 3  is the section view of telescopic disclub joint having elliptical section; FIG.  38 B 4  is the alternative section view of telescopic disclub joint having elliptical section; FIG.  38 C 1  is the interior pole of the telescopic disclub; FIG.  38 C 2  is the interior pole of the telescopic disclub; FIG.  38 D 1  is the pole of the interior pole of the telescopic disclub; FIG.  38 D 2  is the transparent view of the pole of the interior pole of the telescopic disclub; FIG.  38 E 1  is the friction claw mechanism of the interior pole of the telescopic disclub; FIG.  38 E 2  is the transparent version of the friction claw mechanism of the interior pole of the telescopic disclub;  FIG. 38F  is the claw of the friction claw mechanism of the interior pole of the telescopic disclub;  FIG. 38G  is the driving screw of the friction claw mechanism of the interior pole of the telescopic disclub;  FIG. 38H  is the joint of the adjustable angle golf-club style disclub;  FIG. 38I  is the short bar having disclub head for the adjustable angle golf-club style disclub;  FIG. 38J  shows the isotropic view of the disclub head;  FIG. 38K  shows the isotropic view of the disclub head;  FIG. 38L  shows the bottom view of the gripper;  FIG. 38M  shows the side view of the gripper;  FIG. 38N  shows the side view of the gripper;  FIG. 38O  shows the isotropic view of the gripper;  FIG. 38P  shows the isotropic view of the gripper;  FIG. 38Q  shows the golfrisbee having light;  FIG. 38R  shows the section view of the golfrisbee having light;  FIG. 38S  is the adaptor for light packet;  FIG. 38T  shows the isometric view of the light packet of the golfrisbee;  FIG. 38U  shows the screwed adaptor for light adaptor,  FIG. 38V  shows the top view of the light of the golfrisbee;  FIG. 38W  shows the side view of the lighted Disclub and GolFrisbee;  FIG. 38X  shows the grip having the lighted first tube;  FIG. 38Y  shows the lighted first tube;  FIG. 38Z  shows the light packet in the lighted first tube. 
         FIG. 39A  is the wrist-wearing watch monitor for the remote smart phone and video camera;  FIG. 39B  is the system and architecture of power, clock and circuit of the wrist wearing watch monitor and the remote smart phone and video camera. 
       FIG.  40 A 1  is the system and architecture of the jitterless spurfree fast-lock clock for the wrist wearing watch monitor and the remote smart phone and etc.; FIG.  40 A 2  is the circuit of the jitterless spurfree fast-lock clock for the wrist wearing watch monitor and the remote smart phone and etc.;  FIG. 40B  is the system model for the voltage controlled oscillator VCO for the jitterless spurfree fast-lock clock;  FIG. 40C  is the spectrum analysis of the voltage controlled oscillator VCO for the jitterless spurfree fast-lock clock. 
       FIG.  41 A 1  is the timing waveform for the Frequency-Phase Lock Loop FPLL as the frequency of CLK FB  is higher than the CLK REF ; FIG.  41 A 2  is the timing waveform for the Frequency-Phase Lock Loop FPLL as the frequency of CLK FB  is lower than the CLK REF ;  FIG. 41B  is the architecture of Frequency-Phase Lock Loop FPLL;  FIG. 41C  is the frequency waveform of the clock oscillation;  FIG. 41D  is the system and architecture of the jitterless spurfree fast-lock clock Frequency-Phase Lock Loop FPLL. 
         FIG. 42A  is the planar inductor having the magnetic conductor and magnet sensor; FIG.  42 B 1  is the structure of TubeFET; FIG.  42 B 2  is the structure of the inductor having the magnet sensor. 
         FIG. 43A  is the architecture of the rippless and capless smart LDVR Low Drop Voltage Regulator;  FIG. 43B  is the symbol of the nonlinear single side amplifier;  FIG. 43C  is the input and output voltage waveform of the conventional LDVR Low Drop Voltage Regulator;  FIG. 43D  is the input and output voltage waveform of the rippless and capless smart LDVR Low Drop Voltage Regulator. 
         FIG. 44A   1  is the general architecture and system of noiseless green power P&amp;G architecture; FIG.  44 A 2  is the chip level architecture and system of noiseless green power P&amp;G architecture; FIG.  44 B 1  is the characteristic curves of DropLess Voltage Regulator DLVR and DropLess Current Regulator DLIR; FIG.  44 B 2  is the Real DC/DC conversion of the DropLess Voltage Regulator DLVR and DropLess Current Regulator DLIR; FIG.  44 C 1  is the schematics of the DLVR DropLess Voltage Regulator for the saw-tooth voltage input of the switch mode power supply; FIG.  44 C 2  is the waveform of the input of the saw-tooth voltage which is the output of the switch mode power supply and the voltage of the output power of the DLVR DropLess Voltage Regulator; FIG.  44 D 1  is the schematics of the DLIR Low Drop Current Regulator; FIG.  44 D 2  is the alternative schematics of the DLIR DropLess Current Regulator;  FIG. 44E  the board level architecture and system of noiseless green power P&amp;G architecture of the active CM choke implemented with the DropLess Voltage Regulator DLVR and DropLess Current Regulator DLIR;  FIG. 44F  the Power Supply Rejection Ratio PSRR of the Common Mode Choke CM Choke, LDVR and the Active Common Mode Choke ACM Choke;  FIG. 44G  is the power and ground waveforms of the architecture of noiseless Green Power P&amp;G architecture; FIG.  44 H 1  is the power and ground waveform of the conventional digital circuit; FIG.  44 H 2  is the power and ground waveform of the Green Power P&amp;G architecture and system;  FIG. 44I  is the schematics of the DLVR DropLess Voltage Regulator for the high voltage input of the switch mode and/or high voltage dynamic varying power supply. 
         FIG. 45A  is the architecture and system of the analog front for the High Frequency Wireless Sinusoidal Input;  FIG. 45B  is the architecture and system of the analog front for the High Speed Digital Pulse Input. 
         FIG. 46A  is the architecture and system of the conjugate Bandgap Generator made of Bandgap Voltage Generator and Bandgap Current Generator;  FIG. 46B  is the schematics and circuit of the conjugate Bandgap Generator made of Bandgap Voltage Generator and Bandgap Current Generator,  FIG. 46C  is the schematics and circuit of the Bandgap Current Generator;  FIG. 46D  shows the switching mode power for the lighted DisClub Golf. 
         FIG. 47  is the separation/parting line analysis for the conventional disc and golfdisc. 
         FIG. 48  is the aerodynamics analysis of the super-lift golfdisc and conventional disc. 
     
    
    
     DESCRIPTION AND OPERATION 
     The disclub golf has versatile disclubs to play the disclub golf in different ways. To make the golf course compatible, as shown in FIG.  1 D 1 , the disc can throw into a cave as the discolf does. However, as shown in FIG.  1 D 2 A, the best golf course compatible solution is to toss the golfring as the quoits does. The disclub golf uses the golfdisc to throw to avoid the tree blockage. At the last stage, the golfdisc is changed to be the golfring to toss the golfring at the flagpole as the quoits does. As shown in FIG.  1 A 1 , FIG.  1 A 2 , FIG.  1 A 3  and FIG.  1 A 4 , they show the continuous operational pictures of the basic disclub golf. 
     As shown in FIG.  1 A 2 , FIG.  1 A 4 ,  FIG. 4F  and  FIG. 20A , the disclub golf comprises a gliding golfdisc  1  and disclub  2 . The gliding golfdisc  1  comprises a closed rim airfoil  10 . 
     As shown in FIGS.  1 A 2  &amp;  FIG. 33A , the disclub  2  has a straight pole  20 . The disclub head  205  being mounted on the end of said straight pole  20 . 
     As shown in  FIG. 20A ,  FIG. 20B  and  FIG. 20C , the rim airfoil  10  has a substantially right angle triangular cross-section. An outer rounded corner and curved hypotenuse are the upper airfoil edge of the closed rim airfoil  10 . The closed rim airfoil  10  further comprises discap  105 . The disclub  2  further comprises disclub head  205 . The discap  105  rotationally screws on and engages with the disclub head  205 . Swiveling the disclub  2 , due to the eccentric force, the discap  105  and the gliding golfdisc  1  rotates and launches to fly in the sky. 
     The disclub golfer holds the adjustable handle  208  to swivel the disclub  20 . In the FIG.  1 A 1 , the disclub  20  is raised up to be ready to swivel. As shown in FIG.  1 A 2 , the basic disclub  20  is swiveled to the horizontal position. As shown in FIG.  1 A 3 , FIG.  28 A 1 , FIG.  28 A 2 ,  FIG. 29A  and  FIG. 29B , applying the snapping action, the cam locking clip mechanism in the discap  105  and disclub head  205  is suddenly released and the disclub golfdisc  1  rotates very fast 180 degrees. As shown in FIG.  1 A 4 , the disclub golfdisc  1  takes off from the disclub head  205  flying in the sky. As shown in FIG.  14 A 1 ,  FIG. 23B ,  FIG. 30A  and  FIG. 30B , the disclub golfdisc  1  carries the smart phone and video camera. The video signal transmits back to the wristwatch monitor  3 . 
     As shown in FIG.  1 B 2 ,  FIG. 34A  and  FIG. 38I , the golf-style disclub  21  has one end of pole  211  connecting to short bar  213  with one bent joint  212 . The disclub head  205  is mounted on the end of short bar  213 . 
     As shown in FIG.  1 B 1 , FIG.  1 B 2 , FIG.  1 B 3  and FIG.  1 B 4 , they show the continuous operational pictures of the golf-style disclub golf. The golfdisc  10  is mounted on the bent short bar  213  of the golf-style disclub  21 . In the FIG.  1 B 1 , the golf-style disclub  21  is raised up being ready to swivel. As shown in FIG.  1 B 2 , the golf-style disclub  21  is swiveled to the horizontal position. As shown in FIG.  1 B 3 , applying the snapping action, the cam locking clip mechanism in the discap  105  and disclub head  205  is suddenly released and the golfdisc  1  rotates very fast 180 degrees. As shown in FIG.  1 B 4 , the golfdisc  1  takes off from the disclub head  205  flying in the sky. 
     As shown in FIG.  1 C 1 , FIG.  1 C 2 , FIG.  1 C 3 , FIG.  1 C 4 , FIG.  1 C 5 , FIG.  1 C 6 , FIG.  1 C 7 , FIG.  1 C 8 , FIG.  26 D 1 , FIG.  26 D 2 , FIG.  33 C 1 , FIG.  33 C 2 , FIG.  33 D 1 , FIG.  33 D 2 ,  FIG. 35A ,  FIG. 35B , FIG.  36 A 1 , FIG.  36 B 1 , FIG.  36 A 2 , FIG.  36 B 2 , FIG.  36 A 3 , FIG.  36 B 3 ,  FIG. 37C  and  FIG. 37D , the disclub is extendable disclub. The extendable disclub comprises a pole sliding in a tube. The disclub head is mounted on the end of the pole. As shown in  FIG. 35A ,  FIG. 35B , FIG.  36 A 1 , FIG.  36 B 1 , FIG.  36 A 2  and FIG.  36 B 2 , there are callouts to show the cross section of the extendable disclub. In the middle of the extendable disclub, there are elliptical or non-circular sections that the extendable disclub can resist the twist torque of the extendable disclub. 
     As shown in FIG.  1 C 1 , the Tarng golfdisc  11  is mounted on the telescopic disclub  22  in the elongated position. As shown in FIG.  1 C 2 , the telescopic disclub  22  in the shortened position. The pole  222  slides in the tube  221 . The pole  222  is locked with the tube  221  with the locking screw  2212 . The handle  208  is locked to the tube  221 . The Tarng golfdisc  1  is mounted on the disclub head  205  with the discap  105 . As shown in FIG.  1 C 3  and FIG.  1 C 4 , the extendable disclub  27  has the grip  270  mounted on the first tube  271 . The second tube  272  slides inside the first tube  271 . The third tube  273  slides inside the second tube  272 . The disclub head  207  mounts at the end of the third tube  273 , FIG.  1 C 3  is the disclub  27  in the extended position. FIG.  11 C 4  is the disclub  27  in the shortened position. 
     As shown in FIG.  1 D 1 , the golf-style disclub  23  has the angle-adjusted joint  2312  to adjust the launch angle of Tarng disc  11 . The pole  231  has the bent end. The adjusted joint  2312  is mounted on the bent end of pole  231 . The disclub head  205  is mounted on the end bar  232 . In this drawing, the golfrisbee  11  is thrown with disclub into the target hole  11   dk  of the discolf having the flag  11   df.    
     As shown in FIG.  1 D 2 A, the golf-style telescope angle-adjusted disclub  24  comprises the bent pole  242  sliding in the tube  221 . The bent pole  242  is locked to the tube  221  with the locking screw  2212 . The disclub head  205  is mounted on the short bar  232 . The Tarng golfdisc  11  is mounted on the disclub head  205  with discap  105 . As shown in FIG.  1 D 2 B, the bent pole  242  is retracted to be carried easily. The adjusted joint  2312  rotates to turn the short bar  232  to fold the golf-style telescope angle-adjusted disclub  24 . 
     As shown in FIG.  1 E 1  and  FIG. 30A , the telescopic disclub  26  and golfdisc  12  can serve as the self-portrait. The smart phone or camera  151  is mounted on the Tarng golfdisc  12 . The angle-adjusted joint  263  is mounted at the telescopic disclub  26 . The Tarng golfdisc  12  is flipped at the self-portrait position to take the photo and video, etc with the smart phone and video camera  151 . As shown in FIG.  1 E 2 , the Tarng golfdisc  12  is flipped back to the normal disclub swiveling operation position. As shown in FIG.  19 A 1 , the Tarng golfdisc  12  can be the head-wearing golfdisc  18  to wear on the head. The telescopic disclub  26  serves as the Alpenstock as shown in FIG.  1 E 2 . 
     As shown in  FIG. 2A , it is the golf ball-throwing trajectory. The golf ball-launching angle is 45° to have the maximum flying distance. As shown in FIG.  2 B 2 , the golf ball  9  rotates. As shown in  FIG. 2B  and FIG.  2 B 2 , the top airflow is speeded up and the pressure is reduced. As shown in FIG.  2 B 1  and FIG.  2 B 2 , the speed of the bottom airflow is reduced and the pressure is increased. The golf ball floats up due to the pressure difference between the top air and the bottom air. This is referred to be Magnus force. 
     As shown in  FIG. 3A , as the disc  10  flies, the speed reduced and the angle of attack is increased. As shown in FIG.  3 B 1 , the disc  10  flies and rotates. Due to the conservation of the rotational momentum of gyroscopic force, the disc  10  keeps the same orientation. As the disc  10  falls down, the angle of attack becomes much larger. The disc  10  is more like the parachute dropping to the ground. The potential energy of disc  10  does not convert to the dynamic flying energy of the glider. The flying distance of the falling trajectory of the disc  10  is much less than the flying distance of the rising trajectory of the disc  10 . As shown in FIG.  3 B 2 , with the Tarng golfdisc  11 , the rising trajectory and falling trajectory are symmetrical. Therefore, the gliding Tarng golfdisc  11  is more like the glider to be named as the gliding disc. The flying distance of gliding Tarng golfdisc  11  is larger than the disc  10 . 
     As shown in FIG.  4 A 1 , it is the isometric top view of the frictionless super-lift golfdisc  10 . As shown in FIG.  4 A 2 , it is the transparent isometric top view of the frictionless super-lift solar cell golfdisc  1   s . As shown in FIG.  4 B 1 , it is the bottom view of the frictionless super-lift golfdisc  10 . As shown in FIG.  4 B 2 , it is the transparent isometric bottom view of the frictionless super-lift solar cell golfdisc  1   s . As shown in FIG.  4 C 1 , it is the isometric bottom view of the frictionless super-lift golfdisc  10 . As shown in FIG.  4 C 2 , it is the transparent isometric bottom view of the frictionless super-lift solar cell golfdisc  1   s . The discap  105  is embedded in the frictionless super-lift golfdisc  10 . 
     As shown in  FIG. 4D ,  FIG. 4E  and  FIG. 4F , it shows the side view of the frictionless super-lift golfdisc  10 . As shown in  FIG. 20A , the bottom edge  101  of the frictionless super-lift golfdisc  10  is flat. The triangle flap  102  is at the tail end of said bottom edge  101 . The stability edge  103  is to maintain the side stability of the frictionless super-lift golfdisc  10 . However, the stability edge  103  will cause the stagnation point generating the drag force at the trailing edge of the frictionless super-lift golfdisc. 
       FIG. 4E  is the transparent side view of the frictionless super-lift golfdisc  10 . It shows the discap  105  embedded in the triangle rim of the frictionless super-lift golfdisc  10 .  FIG. 4F  is the section view to show the structure of the discap  105  and the dome structure of the frictionless super-lift golfdisc  10 . 
     As shown in  FIG. 4E ,  FIG. 4F , FIG.  6 C 2  and FIG.  6 C 3 , the plateau  1055  inside the discap  105  is to reduce the air flowing into the discap to minimize the air drag force. The hole  1050  embedded inside the plateau  1055  is for the plastic module injection of the golfdisc  10 . The screw  1056  embedded inside the discap  105  is to rotationally mount the discap  105  on the screw  2056  of the disclub head  205  as shown in  FIG. 26A  and  FIG. 26B . 
     As shown in FIG.  5 A 1 , the disc  10  flies with velocity V DISC  and rotates counter-clockwise with V SPIN . The weight of disc  10  is simplified to be the gravity force F G  at the Center Of Gravity CG. All the air pressure force is simplified to be the F LIFT  applied at the Center Of Pressure CP. As the Center Of Pressure CP is located after the Center Of Gravity CG, the lift force F LIFT  generates positive pitch moment MP LIFT . To make the analysis simple with the intuition, due to the gyroscopic force, the lift force F LIFT  and spin V SPIN  generate the equivalent pseudo force PR LIFT  to generate the left banking moment MB LIFT . 
     As shown in FIG.  5 A 2 , the disc  10  flies with velocity V DISC  and rotates counter-clockwise with V SPIN . The weight of disc  10  is simplified to be the gravity force F G  at the Center Of Gravity CG. All the air pressure force is simplified to be the F LIFT  applied at the Center Of Pressure CP. The Center Of Pressure CP is located before the Center Of Gravity CG. The lift force F LIFT  generates negative pitch moment MP LIFT . The lift force F LIFT  and spin V SPIN  generate the pseudo force FR LIFT  to generate the right banking moment MB LIFT . 
     As shown in FIG.  5 B 1 , the disc  10  flies with velocity V DISC  and rotates clockwise with V SPIN . The weight of disc  10  is simplified to be the gravity force F G  at the Center Of Gravity CG. All the air pressure force is simplified to be the F LIFT  applied at the Center Of Pressure CP. The Center Of Pressure CP is located after the Center Of Gravity CG. The lift force F LIFT  generates positive pitch moment MP LIFT . The lift force F LIFT  and spin V SPIN  generate the pseudo force FR LIFT  to generate the right banking moment MB LIFT . 
     As shown in FIG.  5 B 2 , the disc  10  flies with velocity V DISC  and rotates clockwise with V SPIN . The weight of disc  10  is simplified to be the gravity force F G  at the Center Of Gravity CG. All the air pressure force is simplified to be the F LIFT  applied at the Center Of Pressure CP. The Center Of Pressure CP is located before the Center Of Gravity CG. The lift force F LIFT  generates negative pitch moment MP LIFT . The lift force F LIFT  and spin V SPIN  generate the pseudo force PR LIFT  to generate the left banking moment MB LIFT . 
     As shown in  FIG. 5C , it is the trajectory and attitude of the conventional disc. As shown in  FIG. 5C , FIG.  5 C 1  and FIG.  3 B 1 , at the beginning of trajectory, the velocity of disc  10  is fast and the CP is located after CG. The disc  10  rotates clockwise and the disc  10  bank right. The flying distance of the rising trajectory is much longer. As shown in  FIG. 5C , FIG.  5 C 2  and FIG.  3 B 1 , at the end of trajectory, the velocity of disc  10  is slow and the CP is located before CG. The disc  10  rotates clockwise and the disc  10  bank left. The flying distance of the falling trajectory is much shorter. 
     As shown in FIG.  3 B 2 , FIG.  6 A 1 , FIG.  6 A 2 , FIG.  6 B 1 , FIG.  6 B 2  and FIG.  6 C 1 , to enhance the flying distance of disc, the Tarng Disc  11  is adopted. There are many dimples on the rim of the Tarng Disc  11 . As shown in FIG.  6 C 2 , the dimples are concave holes. As shown in FIG.  6 C 3 , the dimples are convex bumps. 
     As shown in FIG.  7 A 1 , the Tarng Disc  11  having the dimples  110  on the rim of disc  11 . The Tarng Disc  11  moves forward with velocity V DISC  and spin counter-clockwise with velocity V SPIN . As shown in FIG.  7 A 1 , on the left side of the Tarng Disc  11 , the air velocity is V AIR +V SPIN . As shown in FIG.  7 A 2 , the air pressure is reduced and there is up-lift force is (+F SPIN ). As shown in FIG.  7 A 1 , on the right side of the Tarng Disc  11 , the air velocity is (V AIR −V SPIN ). As shown in FIG.  7 A 2 , the air pressure increases and there is downward force is (−F SPIN ). Due to the counter-clockwise spin of Tarng Disc  11 , the pseudo-force (+FR SPIN ) and (−FR SPIN ) generate the positive pitching moment MP SPIN . The Tarng Disc  11  banks right. 
     As shown in FIG.  7 B 1 , the Tarng Disc  11  has the dimples  110  on the rim of disc  11 . The Tarng Disc  11  moves forward with velocity V DISC  and spin clockwise with velocity V SPIN . As shown in FIG.  7 B 1 , on the left side of the Tarng Disc  11 , the air velocity is (V AIR −V SPIN ). As shown in FIG.  7 B 2 , the air pressure is increased and there is downward force is (−F SPIN ). As shown in FIG.  7 B 1 , on the right side of the Tarng Disc  11 , the air velocity is (V AIR +V SPIN ). As shown in FIG.  7 B 2 , the air pressure reduces and there is upward force is (+F SPIN ). Due to the clockwise spin of Tarng Disc  11 , the pseudo-force (+FR SPIN ) and (−FR SPIN ) also generate the positive pitching moment MP SPIN . The Tarng Disc  11  banks left. In other words, both clockwise and counter-clockwise rotations generate the positive pitching moment for the parabolic trajectory as shown in FIG.  3 B 2 . 
     As shown in  FIG. 8A , the Tarng Disc  11  has all the forces and moments are included in one picture. The forces and moments are pressure, Tarng Force and weight forces and the momentums generated by the pressure and Tarng force on the flying and rotating disc. The Tarng Disc  11  rotates counter-clockwise. The Center of Pressure CP is located after the Center of Gravity CG. It is noted that both MP LIFT  and MP SPIN  are positive pitching moments. Therefore, the launch angle can be larger than 0°. As shown in FIG.  3 B 2  and  FIG. 9A , the flying trajectory is parabolic and the flying distance is enhanced. The bank moments MB LIFT  and MB SPIN  cancel each other. Therefore, as shown in  FIG. 9C , the Tarng Disc  11  moves forward without tilting as shown in  FIG. 9B . This case is the best performance of the Tarng Disc  11 . Therefore, we try to operate in this case. 
     As shown in FIG.  8 A 2 , the Tarng Disc  11  has all the forces and moments are included in one picture. The forces and moments are pressure. Tarng Force and weight force and the momentums generated by the pressure and Tarng force on the flying and rotating disc. The Tarng Disc  11  rotates counter-clockwise. The Center of Pressure CP is located before the Center of Gravity CG. It is noted that MP LIFT  is negative pitching moment and MP SPIN  is positive pitching moment. The moments MP LIFT  and MP SPIN  cancel each other. Therefore, the launch angle is 0°. Both the bank moments MP LIFT  and MP SPIN  bank right. The Tarng Disc  11  tilts right. Therefore, we try not to operate in this case. This is the launching angle limit for the Tarng Disc  11 . 
     As shown in FIG.  8 B 1 , the Tarng Disc  11  has all the forces and moments are included in one picture. The forces and moments are pressure, Tarng Force and weight force and the momentums generated by the pressure and Tarng force on the flying and rotating disc. The Tarng Disc  11  rotates clockwise. The Center of Pressure CP is located after the Center of Gravity CG. It is noted that both MP LIFT  and MP SPIN  are positive pitching moments. Therefore, the launch angle can be larger than 0°. As shown in FIG.  3 B 2  and  FIG. 9A , the flying trajectory is parabolic and the flying distance is enhanced. The bank moments MP LIFT  and MP SPIN  cancel each other. Therefore, as shown in  FIG. 9C , the Tarng Disc  11  moves forward without tilting as shown in  FIG. 9B . This case is the best performance of the Tarng Disc  11 . Therefore, we try to operate in this case. 
     As shown in FIG.  8 B 2 , the Tarng Disc  11  has all the forces and moments are included in one picture. The forces and moments are pressure, Tarng Force and weight force and the momentums generated by the pressure and Tarng force on the flying and rotating disc. The Tarng Disc  11  rotates clockwise. The Center of Pressure CP is located before the Center of Gravity CG. It is noted that MP LIFT  is negative pitching moment and MP SPIN  is positive pitching moment. The moments MP LIFT  and MP SPIN  cancel each other. Therefore, the launch angle is 0°. The bank moments MP LIFT  and MB SPIN  bank left. Therefore, the Tarng Disc  11  tilts left. Therefore, we try not to operate in this case. This is the launching angle limit for the Tarng Disc  11 . 
     As shown in  FIG. 8A  and FIG.  8 B 1 , the dimples on the top surface of Tarng Disc  11  have the same effect for the clockwise direction and counter-clockwise direction. Therefore, the dimple on the top of Tarng Disc  11  can be the round bump or round cavity which is universal in all directions. 
     As shown in FIG.  10 A 1 , FIG.  10 A 2 , FIG.  10 B 1  and  FIG. B2 , the dimples  120  of Tarng Disc  12  also locate on the bottom plate of the Tarng Disc  12 . However, as shown in  FIG. 11B  and  FIG. 11C , the dimples  120  are uni-directional dimples. There are different lift forces in the right bottom plate and left bottom plate. The lift force is more like the aerofoil lift force. Therefore, the section of the dimple is different to be the uni-directional dimples. 
     As shown in the  FIG. 11B  and  FIG. 11C , the dimple has the unsymmetrical concave. The unsymmetrical concave dimple is similar to the arch of the bottom plate of the aerofoil. It has the different lift forces in the different directions. As shown in  FIG. 11B , the lift force is larger than the lift force as shown in  FIG. 11C . As shown in  FIG. 11A , the (+F SPIN,BOTTOM ) pushes the disc  12  upward and the (−F SPIN,BOTTOM ) pulls the disc  12  downward. Comparing  FIG. 8A  with  FIG. 11A , the (+F SPIN,BOTTOM ) in  FIG. 11A  is the addition to the (+F SPIN ) in FIG.  8 A 1  the (−F SPIN,BOTTOM ) in  FIG. 11A  is the addition to the (−F SPIN ) in FIG.  8 A 1 . 
     As shown in  FIG. 11A ,  FIG. 11B  and  FIG. 11C , on the bottom airfoil edge of the gliding golfdisc has dimples. The dimples on the bottom edge have directional sense. As shown in  FIG. 11A , this is the clockwise Tarng disc  12  having the dimples on the bottom surface of Tarng disc  12 . Being similar to the clockwise Tarng disc  12  in  FIG. 11A , just flip the dimple in the horizontal direction as shown in the  FIG. 11B  and  FIG. 11C , we can have the counter-clockwise Tarng disc. 
     As shown in FIG.  12 A 1 , FIG.  12 A 2 , FIG.  12 B 1 , FIG.  12 B 2  and  FIG. 12C , the super-lift Adaptive Tarng Disc  13  has the adaptive fin  130  to reduce the drag during the glide of the super-lift Adaptive Tarng Disc  13 . The adaptive fin  130  is to reduce the drag force of the stagnation point of the stability edge  103  at the trailing edge of super-lift Adaptive Tarng Disc  13 . The height of the adaptive fin  130  is less than the stability edge  103 . At the side edge of disc  13 , the stability edge  103  serves as the stability fin. The inside curvature  1030  is much larger that the flow will not generate the stagnation point as the stability  103  does. Therefore, the air drag force of disc  13  is reduced. At the front edge, without the adaptive fin  130 , the flow becomes the turbulent flow. The turbulent flow increases the drag force a lot. With the adaptive fin  130 , the flow becomes laminar flow. The air drag force of the laminar flow reduces a lot. 
     As shown in  FIG. 13A ,  FIG. 13B  and  FIG. 13C , the propeller  141  of the discopter  14  is mounted on the triangle shaped rim of the super-lift Adaptive discopter Tarng golfdisc  14 . The super-lift Adaptive discopter Tarng discgolf  14  can wear on head that the super-lift Adaptive discopter Tarng golfdisc  14  can take off from the head. With the adaptive fin  130 , the super-lift Adaptive discopter Tarng golfdisc  14  can wear on head. 
     As shown in FIG.  14 A 1 , FIG.  14 A 2 , FIG.  14 B 1 , FIG.  14 B 2 , FIG.  15 A 1 , FIG.  15 A 2 , FIG.  15 B 1  and FIG.  15 B 2 , the remote surveillance super-lift Adaptive discopter Tarng golfdisc  15  has the smart phone and remote surveillance video camera  151 . The smart phone and remote surveillance video camera  151  takes the video. The wrist monitor  3  or smart phone  3   r  make the remote control for the smart phone and remote surveillance video camera  151 . The video signal is transmitted to the wrist monitor  3  or smart phone  3   r . As shown in FIG.  15 A 2  and FIG.  15 B 2 , the solar cell golfdisc  15   s  provides the electricity to the smart camera  151  and discopter  152 . 
     The earphone and microphone  152  is one curved bracket can hide in the space between the adaptor  130  and stability edge  103 . The disc golfer wears the golfdisc  15  on his head. As the disc golfer wants to speak, the curved bracket pivotally rotates down and the microphone  152  is close to the disc golfer&#39;s mouth to speak. 
     As shown in FIG.  16 A 1 , FIG.  16 A 2 , FIG.  16 B 1 , FIG.  16 B 2 , FIG.  16 C 1  and FIG.  16 C 2 , the remote surveillance super-lift Adaptive discopter Tarng golfring  16  has the smart phone and remote surveillance video camera  151 . The remote surveillance super-lift Adaptive discopter Tarng golfing  16  can wear on head. As shown in FIG.  16 A 2  and FIG.  16 B 2 , the solar cell golfdisc  16   s  provides the electricity to the smart camera  151  and discopter  152 . FIG.  16 C 3  and FIG.  16 C 4  are the discopter serving as for the Head Wearing Device of the Smart Hat of iHat. The adaptor  130  is to have the head to wear the Smart Hat of iHat to take off from the head and land on the head. 
     As shown in FIG.  17 A 1 , FIG.  17 A 2 , FIG.  17 B 1  and FIG.  17 B 2 , the remote surveillance super-lift adjustable Adaptive discopter Tarng golfring  17  has the adjustable adaptive ring  170  to fit the different size head. The adjustable adaptive ring  170  has an opening to adapt the different size of the heads and offering the spring force to clamp the head. As shown in FIG.  17 A 2  and FIG.  17 B 2 , the solar cell golfdisc  17   s  provides the electricity to the smart camera  151  and discopter  152 . As shown in FIG.  17 C 1 , FIG.  17 C 2  and FIG.  17 C 3 , it is the thick golfring  17   a . As shown in FIG.  17 D 1 , FIG.  17 D 2  and FIG.  17 D 3 , it is the thin golfring  17   b . The solar cell s and dimples  110  are on the top surfaces of the thick golfring  17   a  and thin golfring  17   b . The solar cell s and dimples  120  are on the bottom surfaces of the thick golfring  17   a  and thin golfring  17   b . The slat-flap-adaptor  17   sfa  not only serves as the slap and flap but also serves as the head adaptor. The golfring  17   a  and  17   b  can be the smart hat of iHat or discoptor  17  as shown in FIG.  17 A 1  and FIG.  17 B 1 . The smart hat of iHat or discoptor  17  can launch and land on the people&#39;s head. 
     As shown in FIG.  18 A 1 , FIG.  18 A 2 , FIG.  18 B 1  and FIG.  18 B 2 , the remote surveillance super-lift elastic adjustable Adaptive discopter Tarng golfdisc  18  has the top cover  181  to be elastic in the disc form. 
     As shown in FIG.  18 B 2  and FIG.  19 B 2 , the adaptor  181   b  of gliding golfdisc  18  has an opening that the adaptor  181   b  is able to adapt the different size of head. As shown in FIG.  18 A 2  and FIG.  18 B 2 , the solar cell golfdisc  18   s  provides the electricity to the smart camera  151  and discopter  152 . 
     As shown in FIG.  19 A 1 , FIG.  19 A 2 , FIG.  19 B 1  and FIG.  19 B 2 , the remote surveillance super-lift elastic adjustable Adaptive discopter Tarng golfdisc  18  has the top cover  181  to be elastic in the hat form. As shown in FIG.  19 A 2  and FIG.  19 B 2 , the solar cell golfdisc  18   s  provides the electricity to the smart camera  151  and discopter  152 . 
     As shown in  FIG. 20A  and  FIG. 4D , the super-lift disc  10  has the bottom edge  101  to be flat in the horizontal direction. At the trail edge of the bottom edge  101 , the flap  102  is in the right triangle shape with fitting curvatures. The flap  102  makes the super-lift disc  10  having the super-lift. 
     The gliding golfdisc as shown in FIG.  4 A 2  comprises a closed rim airfoil  10  as shown in  FIG. 20A . The rim airfoil  10  has a substantially right angle triangular cross-section with the longer right-angle side being a bottom airfoil edge  101  as shown in  FIG. 20C . An outer rounded corner and curved hypotenuse being upper airfoil edge  100  of the closed rim airfoil  10 . At the rear portion of the bottom edge  101 , the closed rim airfoil  10  further comprises a substantially right triangle flap  102 . As shown in  FIG. 20C , the triangle flap  102  has a longer right-angle side connecting with the bottom airfoil edge  101 . The shorter right-angle side of the rim airfoil  10  and the shorter right-angle side of the triangle flap  102  being in alignment to be one nearly vertical curve  103  of the closed rim airfoil  10 . 
     As shown in  FIG. 20B  and  FIG. 4E , the discap  105  has the bottom edge  101  to be flat. The stability edge  103  is a nearly vertical curve as the conventional disc does. As shown in  FIG. 20C  and  FIG. 4F , to reduce the air drag force, the discap  105  has the plateau  1055 . The plateau  1055  fills up the cavity of the discap  105 . The plateau  1055  prevents the air flowing into the cavity of discap  105 . In the middle of the plateau  1055 , there is a rectangle slot  1050 . During the plastic injection process, the rectangle slot  1050  is to hold the discap  105  to the wall of the plastic module. The screw  1056  is to engage with the screw  2056  of the disclub head  205  as shown in  FIG. 26B . 
     As shown in  FIG. 21A ,  FIG. 21B , FIG.  21 C 1 , FIG.  21 C 2  and FIG.  6 C 1 , is super-lift Tarng golfdisc  11  has the trail triangle flap  102 , curved dome  104  and the dimples  110 . The trail triangle flap  102 , curved dome  104  and the dimples  110  makes the super-lift Tarng golfdisc  11  having the superior flying capability. The anti-thrust stubs  1057  are on the top of discap  105 . As shown in  FIG. 21B , to reduce the air drag to have the long-range drift and glide capability, the curved dome  104  eliminates the stagnation point of the stability edge  103  as shown in  FIG. 20B  and  FIG. 4E . However, the bottom edge of the curved dome  104  is still nearly vertical that it still has the stability function for the golfdisc  11 . 
     As shown in  FIG. 22A ,  FIG. 22B ,  FIG. 22C  and  FIG. 12C , the stability edge  103  is lower than the adaptive fin  130 . The stability edge  103  is to stabilize the disc  13  at the right side and left side of golfdisc  13 . At the rear edge of the golfdisc  13 , the adaptive fin  130  is to reduce the drag force of the stagnation point of stability edge  103 . At the front edge of the disc  13 , the adaptive fin  130  is to reduce the turbulent flow of the stability edge  103 . 
     As shown in  FIG. 21A  and  FIG. 22A , the upper surface of the airfoil rim  13  of the gliding golfdisc has dimples. 
     As shown in FIG.  21 C 2 , the closed rim airfoil of the gliding golfdisc comprises a central section  106  and an annular shoulder  104 . The shoulder  104  decreases in thickness from the rim to the central section  106 . 
     As shown in  FIG. 22C ,  FIG. 12C  and FIG.  16 C 1 , the closed rim airfoil  13  of the gliding golfdisc comprises an adaptor  130 . The adaptor  130  is parallel to the vertical edge  103  of the closed rim airfoil  13 . Between the adaptor  130  and the vertical edge  103 , there is an open space. 
       FIG. 22D ,  FIG. 22E ,  FIG. 22F ,  FIG. 22G  and  FIG. 22H  show the super-lift Tarng golfdisc  15  having the subsonic aerofoil with concave bottom  15   c  and  15   cx . The concave bottom  15   cx  is located on the discap structure  105   x . The concave bottom  15   c  is located on the golfrisbee  15 . The profile of the golfrisbee  15  is in the subsonic aerofoil. 
       FIG. 22I  is the side transparent view of the DisClub Head  205   x  for the super-lift Tarng golfdisc  15  having the subsonic aerofoil with concave bottom  15   cx . The plateau  15   cz  is to fit the concave  15   cx  of the discap  105   x.    
     As shown in  FIG. 22J , the golfrisbee  15  has the structure of bumper-fin-slat  15   s  and wing-fin-flap  102   f  of the aerofoil. 
     The bumper-fin-slat  15   s  is the slat having the functions of (1) slat; (2) fin; and (3) bumper as shown by the arrows. As shown in  FIG. 22J , the bumper-fin-slat  15   s  has the right triangle shape or the right triangle. The front edge is hypotenuse. The bottom edge and the back edge are legs. 
     On the front edge of the golfrisbee  15 , the bumper-fin-slat  15   s  serves as the slat. The air flows through the air gap to increase the lift at the large angle of attack. 
     On the side of the golfrisbee  15 , the bumper-fin-slat  15   s  serves as the fin to provide the side stability. 
     As the golfrisbee  15  hit on the other staff, the bumper-fin-slat  15   s  serves as the bumper providing the hit cushion capability. 
     The wing-fin-flap  102   f  is the flap having the functions of (1) flap; (2) fin; and (3) wing as shown by the arrows. As shown in  FIG. 22J , the wing-fin-flap  102   f  has the right triangle shape or the right triangle. The front edge is hypotenuse. The top edge and the back edge are legs. 
     On the front edge of the golfrisbee  15 , the wing-fin-flap  102   f  serves as the flap. The air flow is deflected downward to increase the lift. 
     On the side of the golfrisbee  15 , the wing-fin-flap  102   f  serves as the fin to provide the side stability. 
     As the golfrisbee  15  hit on the other staff, the wing-fin-flap  102   f  serves as the wing providing the side capability. 
     As shown in  FIG. 22K ,  FIG. 22L  and  FIG. 22M , the wing-fin-flap  102   f  has one option to integrate with the golfrisbee  15 . The bumper-fin-slat  15   s  is piece-wise connected to the golfrisbee  15  with the trunks  15   t , The trunks are short that the air gaps between the golfrisbee  15  and the bumper-fin-slat  15   s  is narrow. 
     As shown in  FIG. 22Q , it shows the module. The discap  105   x  screws on the discap adaptor  105   z . The discap adaptor  105   z  is mounted on the detached ring  15   cz.    
     As shown in  FIG. 23A  and FIG.  17 A 1 , they show the isometric section view of the discopter  17  in the disc-ring shape. As shown in  FIG. 23B  and FIG.  15 A 1 , they show the isometric section view of the smart phone and camera  151  of the remote surveillance super-lift Adaptive discopter Tarng golfdisc  15 . As shown in  FIG. 23C  and FIG.  15 A 1 , they show the isometric section view of the propeller  141  of the discopter for the remote surveillance super-lift Adaptive discopter Tarng golfdisc  15 . The motor  1410  drives the blade  1411  to rotate. 
     As shown in  FIG. 23B , the disc further comprises a smart phone and camera  151 . The smart phone and camera  151  is pivotally mounted on said rim airfoil  15 . 
     As shown in  FIG. 23C , the gliding golfdisc further comprises the propellers  141  to be the discopter. The rim airfoil  15  has multiple cavities. The discopter  141  is embedded in the cavity of the rim airfoil  15 . The discopter  141  has a propeller  1411  mounted on a motor  1410 . The motor  1410  drives the propeller  1411  to rotate. 
     To have the long drive for the disc, being similar to the golf ball hit by the club head, the golfdisc  1  is hit with the disclub head  205 . However, as the disc  1  is launched, the disc  1  is moving. To keep the disc  1  to be fixed on the disclub head  205 , as shown in  FIG. 24A , the cam-locking click point  1051  of the discap  105  is held against the cam-locking click point  2051  of the disclub head  205 . 
     As shown in  FIG. 24B , the discap  105  is clamped between the cam-locking click force of the cam-locking click points  1051  and  2051  and the wedge force of screw tighten between the discap  105  and the club head  205 . The disc  1  and discap  105  are held to the disclub head  205 . The wedge force of the screw tighten force is the tighten force between the discap  105  and the head  205  of disclub. The rotation angle ϕ of the discap  105  on the disclub head  205  is about 165°. 
     As shown in  FIG. 25A  and  FIG. 25B , the click point  1051  is located at the rim of the plateau  1055 . The plateau  1055  eliminates the big hole space of the discap  105 . The rectangle hole  1050  is at the center of the plateau  1055 . It is to hold the discap  105  to the wall of the module for the plastic injection. As shown in  FIG. 25B , between the screw  1056  and the plateau  1050 , there is a rim-type space to fit for the screw  2056  of the disclub head  205  as shown in  FIG. 26A . As shown in  FIG. 25C , the anti-thrust stubs  1057  are on the top of the discap  105 . They absorb the thrust force as the snapping force applied to the discap  105 . The holes  1058  are for the bonding between the disc  1  and the discap  105 . 
     As shown in  FIG. 26A ,  FIG. 26B  and  FIG. 26C , the slope  2058  of disclub head  205  is adapted to the triangle flap  102  of discap  105  as shown in  FIG. 20A . As the disc  1  rotates about 165°, the bottom edge of the discap  105  engages with the flat step  2059  and the triangle flap  102  fits with the slope  2058 . The bottom edge  101  of the discap  105  engages with the flat step  2059  generates the wedge force as shown in  FIG. 24B . The solar cell  205   s  provides the electricity to the smart camera  151  and discopter  152 . As shown in FIG.  26 D 1  and FIG.  26 D 2 , the disclub head  207  has the same screw structure as the disclub head  205  does. As shown in FIG.  33 C 2 , FIG.  33 D 2 ,  FIG. 37C  and  FIG. 37D , the oil ring  2070  is to hold the first tube  271  of the disclub  27  at the shortened position. The grip  270  is mounted on the first tube  271 . As shown in FIG.  33 D 1  and  FIG. 37C , the friction segment  2730  is to hold the tube  273  in the tube  272 . The friction segment  2720  is to hold the tube  272  in the tube  271 . 
     As shown in  FIG. 27B  and  FIG. 29D , the discap and disclub head have a plurality of cam locking clicking point to hold the discap  105  to the disclub head  205 . The cam locking clicking point  1051  is attached to inner wall of the discap  105 . The cam locking clicking point  2053  is attached to the outer wall of the disclub head  205 . 
     FIG.  29 E 1  shows the discap  105  embedded in the golfrisbee  11 . FIG.  29 E 2  shows the cave of the discap  105   z  embedded in the golfrisbee after the discap  105   z  being removed. FIG.  29 E 3  shows the bottom view of the discap  105 . FIG.  29 E 4  shows the top view of the discap  105   x  having the anti-shock stubs. FIG.  29 E 5  shows the top view of the discap  105   z  having the concave structure for the plastic injection to reduce the shrinkage. FIG.  29 F 1  shows the adaptable discap  105   a  embedded in the golfrisbee. The adaptable discap  105   a  is removable to change for the different adaptable discaps  105   a . FIG.  29 F 2  shows the bottom isotropic view of the adaptable discap  105   a . FIG.  29 F 3  shows the top view of the adaptable discap  105   ax  having the anti-shock stubs, FIG.  29 F 4  shows the cave of the adaptable discap  105   ax  embedded in the golfrisbee after the adaptable discap being removed for the discap as shown in FIG.  29 F 3 . FIG.  29 F 5  shows the top view of the adaptable discap  105   az  having the concave structure for the plastic injection to reduce the shrinkage. FIG.  29 F 6  shows the cave of the adaptable discap  105   az  embedded in the golfrisbee after the adaptable discap  105   az  being removed for the discap as shown in FIG.  29 F 5 , FIG.  29 G 1 , FIG.  29 G 2  FIG.  29 H 1  and FIG.  29 H 2  the foil stamping of golfrisbee. 
     As shown in  FIG. 27A  and  FIG. 27B , they show the single cam-locking clicking point structure.  FIG. 27A  shows the single cam-locking clicking point  1051  and cam-locking clicking point  2051  being in the lock position.  FIG. 27B  shows the single cam-locking clicking point  1051  and cam-locking clicking point  2051  being in the release position. The solar cell  205   s  provides the electricity to the smart camera  151  and discopter  152 . 
     To adjust the flying distance of the disc, we can adjust the snapping force with the multiple cam-locking clicking points. As shown in FIG.  28 A 1  and FIG.  28 B 1 , they show the discap  105  having the multiple cam-locking click points,  1051 ,  1052  and  1053 . As shown in FIG.  28 A 2  and FIG.  28 B 2 , they show the disclub head  205  having the multiple cam-locking click points,  2051 ,  2052  and  2053 . As shown in  FIG. 29A  and  FIG. 29B , they show the cam-locking clicking point structure.  FIG. 29A  shows the cam-locking triple clicking point in the release position.  FIG. 29B  shows the cam-locking triple clicking point at the single lock position having one click point in the lock position.  FIG. 29C  shows the cam-locking triple clicking point at the double lock position having two click points in the lock position.  FIG. 29D  shows the cam-locking triple clicking point at the triple lock position having three click points in the lock position. 
     As shown in FIG.  29 E 1  and FIG.  29 E 2 , it is the isotropic bottom view of the golfrisbee  11  having the discap  105  or discap  105   z  embedded in the golfrisbee  11 . The discap  105  or discap  105   z  cannot be removed from golfrisbee  11 . 
     On the contrary, as shown in FIG.  29 F 1 , it is the isotropic bottom view of the golfrisbee  11   a  having the discap  105   a  mounted on the golfrisbee  11   a . The discap  105   a ,  105   ax  or  105   az  can be removed from the golfrisb  11   a . FIG.  29 F 4  is the isotropic bottom view of the golfrisbee  11   ax  as the discap  105   ax  is removed from the golfrisbee  11   ax . FIG.  29 F 6  is the isotropic bottom view of the golfrisbee  11   az  as the discap  105   ax  is removed from the golfrisbee  11   az.    
     As shown in FIG.  29 G 1 , FIG.  29 G 2 , FIG.  29 H 1 , FIG.  29 H 2 ,  FIG. 29I  and  FIG. 29J , are the logos print on the golfrisbee,  FIG. 29K  is the symbol of the Professional DisClub Golf Association (PDCGA). 
     As shown in  FIG. 30A  and  FIG. 30B , the smart phone  151  comprises the versatile vision facilities  1512  and  1513  such as camera, holographic projector light, laser, speaker, antenna and infrared, etc. As shown in  FIG. 23B , the smart phone  151  is mounted on the golfdisc  1  with the pivotal axis  1511 . 
     As shown in  FIG. 31A  and  FIG. 31B , the discopter  141  has the propeller  1411  mounted on the motor  1410 . As shown in  FIG. 23C  and  FIG. 30A , the propeller  141  of discopter  15  is mounted in the frame of golfdisc rim. 
     As shown in  FIG. 32A ,  FIG. 32B , FIG.  1 E 1  and FIG.  1 E 2 , the golfdisc  12  and disclub  26  can serve as the self-portrait with the camera of smart phone  151 . As shown in FIG.  32 D 1  and FIG.  32 D 2 , the disclub head  205  is mounted a pivotal joint  206 . As shown in FIG.  32 C 1 , FIG.  32 C 2 , FIG.  32 D 1 , FIG.  32 D 2 , FIG.  32 E 1 , FIG.  32 E 2  and  FIG. 32F , pulling the cam handle  2632  to rotate on the pixel  26311  to release the lock axle  2631 . Pushing the cam handle  2632  to rotate on the pixel  26311 , the cam  26310  engages with the fork  2630  to pull the lock axle  2631 . As shown in  FIG. 32F , the slope  26313  of the lock axle  2631  pushes the slope  20603  of the club head block  2060  to engage the club head block  2060  with the fork  2630 . 
     As shown in  FIG. 33A  and  FIG. 33B , the disclub  20  has the grip  208  and the club head  205 . The disclub head  205  is mounted on the disclub head tube  203 . As shown in FIG.  38 A 1  and FIG.  38 A 2 , the grip  208  has the clamping ring  2082  and the cam handle  2081 . Pushing the cam handle  2081 , the cam at the top of the cam handle  2081  will push the  2082  to lock the handle  2081  to the club  20 . As shown in FIG.  33 C 1 , FIG.  33 C 2 , FIG.  33 D 1 , FIG.  33 D 2 ,  FIG. 37C  and  FIG. 37D , the extendable disclub  27  adopts the friction segments  2720  and  2730  to hold the extendable disclub  27  in the extended position. The friction force is strong enough to resist the twisting torque of the disclub  27 . This twisting torque is generated by the swivel of the disclub to launch the disc  207  to fly. 
     As shown in  FIG. 34A  and  FIG. 34B , the golf-club style disclub  21  has the handle  208  and the club head  205 . The disclub head  205  is mounted on the disclub head tube  203 . As shown in  FIG. 35A , FIG.  36 A 1 , FIG.  36 A 2  and FIG.  36 A 3 , the telescopic disclub  22 ,  22   e  and  22   f  are is in the elongation position. As shown in the  FIG. 35A  and FIG.  36 A 1 , the callouts show the cross sections of the extendable disclub  22   e . The disclub tube  221   e  and disclub pole  222   e  have the smooth transition between the circle and elliptical or non-circular cross sections. The elliptical or non-circular section of the disclub tube  221   e  and disclub pole  222   e  at the joint portions can resist the twist torque during the swivel of the disclub. The long/major axis of the elliptical or non-circular cross section is transverse the swivel direction of the extendable disclub  22   e . As shown in  FIG. 35A  and FIG.  36 A 1 , the bulk  2212   e  is optional. The bulk  2212   e  can strengthen the joint to resist the twist torque during the swivel of the disclub  22   e . As shown in FIG.  38 B 3  and FIG.  38 B 4 , the extended pole  222   e  and tube  221   e  have the elliptical and non-circular section. The tube  221   e  has one cavity  221   c . The pole  222   e  has one bump  222   b . The bump  222   b  fits in the cavity  221   c  to lock the pole  222   e  with the tube  221   e . The knotch  222   k  is to increase the elasticity of the operation of the bump  222   b  and the cavity  221   c . As shown in  FIG. 35B , FIG.  36 B 1 , FIG.  36 B 2  and FIG.  36 B 3 , the telescopic disclub  22 ,  22   e  and  22   f  are in the shortened position. As shown in FIG.  36 A 2  and FIG.  38 B 2 , the screw  2212  is screwed on the tube  221  to tighten the pole  222 . As shown in FIG.  36 A 2 , all the callouts have the circle sections. To resist the twist torque, the friction craw  2215  is adopted. As shown in FIG.  36 A 2 , all the callouts of disclub  22  are circular cross sections view. It needs the self-tighten mechanism of friction craw  2215  to resist the twist torque. The length of disclub  22  can be adjusted freely. As shown in FIG.  36 A 3  and FIG.  36 B 3 , the torque free disclub  22   f  has no torque during the swivel of disclub  22 . The extend pole  222   f  has one bend that the disclub head  205  is aligned with the centerline  22   fc  of the torque free disclub  22   f . Since the disclub head  205  is aligned with the centerline  22   fc  of the torque free disclub  22   f , the torque is very small during the swivel of the torque free disclub  22   f.    
     As shown in FIG.  38 C 1 , FIG.  38 C 2 , FIG.  38 D 1 , FIG.  38 D 2 , FIG.  38 E 1 , FIG.  38 E 2 ,  FIG. 38F  and  FIG. 38G , the friction craw  2215  is constituted of the craw  22152  and the driving screw  22151 . The driving screw  22151  drives the claw  22152 . The friction craw  2215  biases against the internal wall of the tube  221 . Rotating the pole  222  to disengage the lock between the pole  222  and the tube  221 , the pole  222  can slide inside the tube  221 . Rotating the pole in the reverse direction to engage the lock between the pole  222  and the tube  221 , the pole  222  is locked with the tube  221 . This is the internal lock. Furthermore, there is the external lock. As shown in FIG.  38 B 1 , FIG.  38 B 2  and FIG.  36 A 2 , the screw  2212  locks the internal sliding pole  222  with the external tube  221 . This is the external lock. With both the internal lock and external lock, the sliding pole  222  can be locked to the tube  221  firmly to be the discgolf stick. 
     Referring to FIG.  38 C 1 , FIG.  38 C 2  and  FIG. 37A , due to the twisting moment, the telescopic disclub  22  has the self-tighten feature to be the right-hand telescopic disclub  22 R as shown in  FIG. 37A  and left-hand telescopic disclub  22 L as shown in  FIG. 37B . 
     As shown in  FIG. 37A , the extendable disclub  22 R is right-hand disclub having the left-hand locking screw  2212 L and  2215 L. All the callouts have the circular cross sections. The disclub head  205 R is right-hand screw. 
     As shown in  FIG. 37A , swiveling the right-hand telescopic disclub  22 R, the twisting momentum is left-hand momentum. The friction screw  2215 L and the screw  2212 L are left-hand screw to have the self-tighten effect. 
     As shown in  FIG. 37B , the extendable disclub is left-hand disclub having the right-hand locking screw  2212 R and  2215 R. All the callouts have the circular cross sections. The disclub head  205 L is left-hand screw. 
     As shown in  FIG. 37B , swiveling the left-hand telescopic disclub  22 R, the twisting momentum is right-hand momentum. The friction screw  2215 R and the screw  2212 R are right-hand screw to have the self-tighten effect. 
     Being similar to  FIG. 32A  and  FIG. 32B , the U-joint  2312  is made of the U-fork  263 J and pivotal head  205 J as shown in  FIG. 38H . As the cam handle  2632 J is pushed down to lock the U-joint  2312 , the pivotal block  2060 J biases against the wall of U-fork  263 J. As shown in FIG.  1 D 2 A,  FIG. 38H  and  FIG. 38I , the end bar  232  is mounted on the joint end  205 J,  FIG. 38J  and  FIG. 38K  show the isotropic view of the disclub head.  FIG. 38L ,  FIG. 38M ,  FIG. 38N ,  FIG. 38O  and  FIG. 38P  show the bottom, side and isotropic views of the gripper  270 . 
     The light DisClub Golf is for the night golf and entrainment. Both the disclub and Golfrisbee can be implemented with the addition of either Fluorescent agent or Phosphor. As shown in  FIG. 38W , the light DisClub Golf comprises the light DisClub  2 L and the light GolFrisbee  1 L. As shown in  FIG. 38W ,  FIG. 38Q  and  FIG. 38R , the lighted golfrisbee  1 L has the discap  105  and light LED  106 . As shown in  FIG. 38T , the battery  106   b  installed in the light packet  106   p . The light packet  106   p  has the toggling switching button  106   s  and the LED lights  106   d . The toggling switch  106   s  turns on and turns off the LED  106   d . As shown in the  FIG. 38T , the light packet  106   p  is installed in the light screw  106   u . The light screw  106   u  is screwed in the light LED adaptor  106   v . As shown in  FIG. 38Z , the grip mounted on the lighted first tube  271 L. The toggling switch  271   s  turns on and turns off the LED  271   d . The battery  271   b  is installed in the light packet  271   p . As shown in  FIG. 46D , the switch SW can be either the toggling switching button  106   s  and the toggling switch  271   s . The battery BAT can be either the battery  106   b  or the battery  271   b . As the switch SW is turned on, the Switch Mode Power Supply light up the LED. The LED can be either the LED  106   d  or the LED  271   d.    
     As shown in  FIG. 39A  and FIG.  14 A 1 , the wrist-wearing video monitor  3  has the video  31  displayed on the flexible film  30 . As shown in  FIG. 39B  and  FIG. 23B , the architecture of the head wearing smart phone wireless camera  151  and the video monitor  3  has the DropLess Voltage regulator DLVR, DropLess Current Regulator DLIR, Frequency Phase Lock Loop FPLL, Radio Front RF, Analog Front AF and Inductor Capacitor Oscillator LCO, etc. As shown in FIG.  40 A 1 , FIG.  40 A 2 ,  FIG. 40B  and  FIG. 40C , it is the operation of the LC oscillator LCO. The inductor L 1  in FIG.  40 A 2  might be implemented with the inductor as shown in  FIG. 42A . As shown in FIG.  41 A 1 , FIG.  41 A 2 ,  FIG. 41B ,  FIG. 41C  and  FIG. 41D , it is the operation of the FPLL. 
     The conventional concept of the phase noise is completely wrong. The clock oscillation is
 
 fclk ( t )= B+A  sin(ω t +ο( t ))
 
     Assuming no phase noise, ϕ(t)=0
 
 fclk ( t )= B+A  sin(ω t )
 
ω=2π/( LC   TUNE ) 1/2  
 
     To completely specify the sinusoidal oscillation of the clock, we need one set having four parameters, [L, C, A, B]. 
     However, the conventional LCO design has only [L, C] two parameters. 
     From the following equations, they show the variance of the amplitude ΔA and the wandering variance of the baseline/center line ΔB will generate the phase noise ϕ(t). 
     
       
         
           
             
               
                 
                   
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                               ϕ 
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                   = 
                     
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                         B 
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                           Δ 
                           ⁢ 
                           
                               
                           
                           ⁢ 
                           B 
                         
                       
                       ) 
                     
                     + 
                     
                       
                         ( 
                         
                           A 
                           + 
                           
                             Δ 
                             ⁢ 
                             
                                 
                             
                             ⁢ 
                             A 
                           
                         
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                       ⁢ 
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                       ⁢ 
                       
                           
                       
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     The variance of [A, B] becomes the phase noise.
 
ϕ( t )=sin −1 {[Δ B+ΔA  sin ω t ]/ A} 
 
     From the above equation, as ΔA=0 and ΔB=0, the phase noise ϕ(t)=0. In other words, to clean out the phase noises, we need to specify the four parameters, [L, C, A, B] to have the ΔA=0 and ΔB=0. 
     The amplitude A and baseline B can also be measured with the
         A PEAK : maximum value of A   A VALLEY : minimum value of A
 
 A =( A   PEAK   −A   VALLEY )/2
 
 B =( A   PEAK   +A   VALLEY )/2
       

     As shown in FIG.  40 A 1  and FIG.  40 A 2 , the oscillator has the Common Mode FeedBack CMFB, B=const, feedback “−ΔB” to cancel the “ΔB” noise. The oscillator has the Constant Amplitude FeedBack CAFB, A=const, feedback “−ΔA” to cancel the “ΔA” noise. 
     As shown in  FIG. 40B , it is the mathematical model of the noiseless LCO. The LCO generates f osc  as shown in the curve of f osc −f in  FIG. 40C . The local oscillator generates frequency δ(f o ). The local oscillator frequency δ(f o ) mixes with the LCO output f osc . As shown by the curve f noise −f in  FIG. 40C , the mixture of the output passes the low pass filter LPF to get the −f noise . The −f noise , feedbacks to cancel the f noise . 
     As shown in FIG.  41 A 1  and FIG.  41 A 2 , they show the waveforms of the operation of the FPLL Frequency-Phase Lock Loop.  FIG. 41B  shows the architecture of the controller of the FPLL Frequency-Phase Lock Loop. As shown in  FIG. 41D , the complete FPLL is constituted of the FPLL controller and the OSC oscillator as shown in  FIG. 40A . 
     As shown in  FIG. 41C , the dotted line is the output frequency of the conventional PLL phase lock loop. The solid line is the output frequency of FPLL. The settling time of the FPLL frequency phase lock is much faster than the conventional PLL. As shown in  FIG. 41D , the counter is served as the FLL frequency detector. As shown in  FIG. 41B , as the counter finishes count N, the CLK FB  is generated. The phase detector is only serves as the PLL phase detector. 
     As the counter is counted to the preset value N, the counter is reset for the next cycle of frequency count. At beginning of the count, the oscillator has the injection lock synchronization to synchronize the input reference clock with the oscillator. As shown in FIG.  41 A 1 , the oscillation comes earlier than the reference clock; the Inject Lock Synchronization makes the synchronization of the reference clock and the oscillator immediately. As shown in FIG.  41 A 2 , the oscillation comes later than the reference clock; the Inject Lock Synchronization makes the synchronization of the reference clock and the oscillator in the next cycle of the reference clock. As shown in  FIG. 41B , FIG.  41 A 1  and FIG.  41 A 2 , the SyncGate is to control the synchronization of the reference clock and the oscillator. 
     As shown in  FIG. 42A , the planar magnet  40  has the magnet conductor loop  41  and magnet sensor  401 . As shown in  FIG. 42B   1 , it is the nanometer TubeFET having the gate G, source S and drain D. The conducting channel between the source S and gate D is completely surrounding and embedded in the gate G. Being similar to the TubeFET, as shown in FIG.  42 B 2 , the Smart Coil has the magnet coil completely surrounds and driving the magnet sensor  401 . The magnet sensor  401  has the similar structure of TubeFET.  FIG. 43A  shows the smart capless LDVR Low Drop Voltage Regulator having the transient &amp; static loop and the dynamic switch loop. As the output voltage Vo is less than the specified voltage, the input terminals of the linear amplifier is short. The transient &amp; static Loop is equivalent to the nonlinear amplifier as shown in  FIG. 43B . For the switching current of the digital circuit, the dynamic switch loop has the fast closed loop. During the voltage sink of the digital circuit switching, the capacitor C SWITCH  switches on the P-type switch to pull down the gate of PFET to charge the output. 
     As shown in  FIG. 43C , the output voltage Vout of the conventional LDVR has the ripple. The in-rush current is very high. The voltage sink of the digital circuit switching is very large. 
     As shown in  FIG. 43D , the output voltage Vout of the smart LDVR rises slowly and smoothly. The in-rush current is very small. The voltage sink of the digital circuit switching is very small. 
     As shown in  FIG. 39B  and FIG.  44 A 1 , the gliding golfdisc has smart phone and camera comprises the general green power architecture made of dropless voltage regulator DLVR and dropless current regulator DLIR. A capacitor C SW connects  between the input of the dropless current regulator DLIR and the input of dropless voltage regulator DLVR. 
     As shown in FIG.  44 A 2 , the chip level green P&amp;G architecture is constitute of the DLVR DropLess Voltage Regulator and DLIR DropLess Current Regulator. 
     As shown in  FIG. 39B , FIG.  44 A 1  and FIG.  44 A 2 , the gliding golfdisc wherein smart phone and camera comprises green power architecture made of dropless voltage regulator DLVR and dropless current regulator DLIR. A passive charging capacitor C SW  connected between an input of said dropless current regulator DLIR and an input of said dropless voltage regulator DLVR. The dropless current regulator DLIR filters out the switching circuit noise in ground to be current noises ΔI. The passive charging capacitor C SW  converts the current noises ΔI in the ground node to be the voltage noises ΔV in power node. Instead of the conventional active voltage charge pumping process, this is the passive current charge pumping process. The voltage noises ΔV DD  filtering with said dropless voltage regulator DLVR to be voltage potential energy of clean power supply. 
     As shown in FIG.  44 A 1 , FIG.  44 B 1  and FIG.  44 B 2 , the DLVR DropLess Voltage Regulator has the output voltage to be the constant voltage V CC . This is the real DC/DC process. The DLIR DropLess Current Regulator has the output current to be the constant current I SS . The CKT circuit generates the current I SS +ΔI. Due to the DLIR, the I SS  flows through the ground inductor. From L(dI/dt)=L(dI SS /dt)=0, the Gnd voltage is the same voltage as PAD_Gnd to be 0V. Due to the buck converter type DLIR Dropless effect caused by the ground inductor, the VSS is 0V. 
     Comparing FIG.  44 A 2  with  FIG. 44E , FIG.  44 A 2  is the chip version of Green Power P&amp;G architecture and system.  FIG. 44E  is the board version of Green Power P&amp;G architecture and system. 
     As shown in FIG.  44 A 2 , it is the detailed design of the chip version green power P&amp;G architecture and system. The Analog circuit and digital circuit are separated. The switching current noise ΔI generated by the digital circuit injects into the switching capacitor C SW . The switching current ΔI of ground node is converted to the switching voltage ΔV of the power node. This behavior is similar to the charge pump circuit. Instead of using the voltage mode as the active drive circuit of charge pump does, the passive circuit switching circuit use the current mode ΔI to do the current charge pump. 
     The switching current ΔI injects into the switch capacitor C SW  to be ΔV. All the switching noise energy injecting into V DD  to store in the power inductor L_V DD . The switching mode power and the switching noise power add up to be the switch power. The switch power going through the DropLess Voltage Regulator DLVR to be the clean power having the constant voltage V CC . The switch noise energy is recycled to be the useful power. The parametric inductor L_V DD  serves as the switching energy storage in the dynamic oscillatory form. 
     As shown in  FIG. 43A , FIG.  44 C 1 , FIG.  44 C 2  and FIG.  44 B 2 , the Low Drop Voltage Regulator LDVR has the voltage drop. The DropLess Voltage Regulator DLVR does not have the voltage drop due to the DLVR has the hybrid operation of the buck-boost-LDVR type inductor operation. 
     The DropLess Voltage Regulator DLVR has the average of the switch mode power voltage due to the extra inductor as shown in FIG.  44 C 1 . The DLVR DropLess Voltage Regulator is the active RC filter to be rippless and capless. As shown in  FIG. 44I , the DropLess Voltage Regulator DLVR is for the dynamic varying high voltage input V HIGH . The resistor R has the dual purposes. The first purpose is to shut down the output device M POUT  during the power up transient process. The second purpose is to move the third poles to very high frequency to have the same stability as the two-poles system does. Therefore, the stability of the three-poles system is the same as the conventional two-poles LDVR Low Drop Voltage Regulator system does. 
     As shown in FIG.  44 B 2  and FIG.  44 C 2 , the waveform of the input of the saw-tooth voltage output of the switch mode power supply is converted to the constant potential voltage of the output power with the active RC filter rippless and capless DLVR Low Drop Buck converter Voltage Regulator. 
     As shown in FIG.  44 B 1 , FIG.  44 D 1  and FIG.  44 D 2 , the chip version DLIR DropLess Current Regulator uses the parametric inductor L_Gnd to be the current sensor. The capacitor CJ is to keep the V GS  of output NMOS type device to be constant to regulate the current to be constant. The differential amplifier senses the voltage variance ΔV caused by the variance of the current ΔI. 
     As shown in  FIG. 44E , the active Common Mode Choke CM choke is implemented with the DropLess Voltage Regulator DLVR and DropLess Current Regulator DLIR. It is the board version of the green power architecture. It is the merge of the DLVR in  FIG. 44C   1  with the DLIR in FIG.  44 D 1 . 
     As shown in  FIG. 44F , the Power Supply Rejection Ratio PSRR of the LDVR has the band-limited frequency in low frequency. The PSRR of conventional Common Mode choke, CM choke, has the band-limited frequency in the high frequency. The PSRR of the Active Common Mode choke, ACM-Choke, has no band limited. The ACM-Choke combines the PSRR of both LDVR and CM Choke to be the flat curve which has no band-limited. The noisy input power VDD is connected to the DLVR as input power. The output of the DLVR is the clean power VCC. The noisy input ground GND is connected to the DLIR. The output of the DLIR is the clean ground VSS. 
     As shown in FIG.  44 A 1 , FIG.  44 A 2  and  FIG. 44E , the Green Power Architecture and System has the voltage waveforms of V DD , V CC , V SS  and Gnd as shown in  FIG. 44G . 
     As shown in  FIG. 44H   1 , the SPICE simulation result of the conventional circuit has the waveforms of power VDD and ground GND oscillate violently having the amplitude +/−93 mv. 
     As shown in FIG.  44 A 1 ,  FIG. 44A   2 ,  FIG. 44E  and FIG.  44 H 2 , with the green power architecture and system of recycling energy, the SPICE simulation result shows the noise amplitudes of VCC, VSS and GND are reduced to be +/−0.05 mV. The noise reduction is 32.7 dB. However, the amplitude of VDD is almost double, +/−160 mV. All the noises in the ground GND is injected and stored in the power VDD. Then the noisy power VDD is filtered to be clean power VCC with the DLVR DropLess Voltage Regulator. 
       FIG. 45A  shows the analog front of the high frequency wireless cellular phone.  FIG. 45B  shows the high-speed analog front of the digital communication system. It shows the high frequency wireless system and the high-speed digital circuit. The high-frequency wireless system uses the root-mean-square RMS detector to detect the power to adjust the Variable Gain Amplifier VGA. The high-speed digital circuit uses the peak detector to detect the amplitude to adjust the Variable Gain Amplifier VGA. The comparator of the high-speed digital circuit can be considered as the 1-bit ADC of the high-frequency wireless system. 
     As shown in  FIG. 46A  and  FIG. 46B , the gliding golfdisc comprises the smart phone and camera having bandgap generator BG. The bandgap generator BG further comprises a voltage bandgap generator V BG  and current bandgap generator I BG . The voltage bandgap generator V BG  generates I PTAT  current and V BG  bandgap voltage and feeding them into the current bandgap generator I BG . The current band generator I BG  generates the bandgap current I BG  and feeding it into the voltage bandgap generator V BG . 
     As shown in  FIG. 46A ,  FIG. 46B  and  FIG. 46C , the bandgap voltage V BG  is generated by the bandgap generator BG. The BG Bandgap Generator is constituted of the voltage bandgap generator V BG  Gen and the current bandgap generator I BG  Gen. The voltage bandgap generator V BG  Gen sends the voltage V BG  and the current I PTAT  to current bandgap generator I BG . The current bandgap generator I BG  Gen sends the bandgap current to the voltage bandgap generator V BG  Gen. As shown in  FIG. 46C , the current flows through bipolar device Q 1  is I PTAT  and the voltage across the bipolar device Q 1  is V CTAT . Therefore, the current flowing through R 3A  is I CTAT . With the adjustment of R 3A , the current flowing through R 1A  is the bandgap current
 
 I   BG   =I   PTAT   +C   TAT .
 
     The currents flowing through R 2A  and R 2B  are the nonlinear compensation for the logarithm factor of the V CTAT . 
     As shown in  FIG. 47 , the Separation/Parting line of disc determines the performance of disc. The lower the Separation/Parting line is, the more lift is and the less stability is. The higher the Separation/Parting line is, the less lift is and the more stability is. To break the rule, the golfdisc adopts the flat bottom with the tail flap. It has the maximum lift and the maximum stability. 
     As shown in  FIG. 48 , the solid line is the flow trajectory of the golfdisc. The dotted line is the conventional disc. At the front portion, the tail flap has the higher lift. For the golfdisc, the flow hits the rear portion of the dome area. For the conventional disc, the flow hits the front portion of the dome area. Therefore, the Center of Pressure CP of the golfdisc is located after the Center of Pressure CP of conventional disc. Therefore, the stability of the golfdisc is more stable than the conventional disc does. At the rear portion, for the golfdisc, due to the tail flap, the airflow bypasses the flat bottom and the cavity of the discap  105 . For the conventional disc, the air blows into the cavity of discap  105 . Therefore, the drag of golfdisc is much less than the conventional disc. At the side of disc  10 , the golfdisc flap has more stability than the conventional disc without the flap. Therefore, the disc with the flap is the biggest innovation in the disc golf. 
     The camera, video display and monitor have the green power architecture made of the DLVR DropLess Voltage Regulator, DLIR DropLess Current Regulator and Switch Noise Power Charging Capacitor to convert the noise energy to be the useful power. The camera, video display and monitor further have the Bandgap Generator being constituted of the Voltage Bandgap Generator and Current Generator. The Frequency-Phase Lock Loop comprises the frequency lock and phase lock two stages and the frequency lock is implemented with the counter. The DropLess Voltage Regulator DLVR is implemented with the hybrid combination of the LDVR and P-side buck type inductor. The DropLess Current Regulator DLIR is implemented with the sense of voltage difference of the parasitic inductor induced by the variance of the current. The active common mode choke ACM is made of the common mode choke, the DLVR DropLess Voltage Regulator, DLIR DropLess Current Regulator and Switch Noise Power Charging Capacitor. 
     While the invention has been particularly shown and described with reference to the preferred embodiments thereof, it will be understood by those skilled in the art that various changes in form and details may be made therein without departing from the spirit and scope of the invention. It is noted that this disclub golf design can be easily modified to be the left-handed ultra-long-drive disc and disclub with the right-hand screws changing to be the left-hand screws. Furthermore, it is noted that the discap and head positions can be interchangeable for disclub and golfdisc. In other words, even in the previous description, all the discussion is based on the alignment of the disclub head  10  being on disclub  1  and the discap  20  is on golfdisc  2 . However, the alignment of the fitting discap is on disclub and the head is on golfdisc is also workable. The same principles and methodologies, etc are applicable to both cases. All the innovations made for the golfdisc of disclub golf can be applied to the conventional disc of disc golf, too.