Source: http://www.google.es/patents/US20010020936?dq=flatulence
Timestamp: 2013-05-24 16:54:19
Document Index: 631173701

Matched Legal Cases: ['art 23', 'art 23', 'art 23', 'art 23', 'art 23', 'art 23', 'art 23', 'art 23', 'art 23', 'art 23', 'art 23', 'art 23']

Patente US20010020936 - Coordinate-capturing apparatus - Google PatentesB�squeda Im�genes Maps Play YouTube Noticias Gmail Drive M�s » B�squeda avanzada de patentes | Historial web | Iniciar sesi�n B�squeda avanzada de patentesPatentesA coordinate-capturing apparatus suitable for inputting handwritten characters or diagrams to a computer or a printer is disclosed. The apparatus includes an ultrasonic transmitter mounted on an input pen for transmitting ultrasonic waves, two ultrasonic receivers for receiving ultrasonic waves transmitted...http://www.google.es/patents/US20010020936?utm_source=gb-gplus-sharePatente US20010020936 - Coordinate-capturing apparatus N�mero de publicaci�nUS20010020936 A1Tipo de publicaci�nSolicitud Fecha de publicaci�n13 Sep 2001 Fecha de presentaci�n8 Feb 2001 Fecha de prioridad21 Feb 2000Tambi�n publicado comoEP1128319A1US7336262US20030197692 N�mero de publicaci�nUS 2001/0020936 A1US2001/0020936A1 InventoresKenzo Tsuji Cesionario originalTsuji Kenzo Clasificaci�n de EE.UU.345/177345/173 Clasificaci�n internacionalG06F3/043G01B17/00G06F3/033G01S5/20 Clasificaci�n cooperativaG06F3/03545G06F3/043 Clasificaci�n europeaG06F3/0354NG06F3/043Referencias Citada por (1)Enlaces externosUSPTO Cesi�n de USPTO EspacenetCoordinate-capturing apparatusUS 20010020936 A1 Resumen A coordinate-capturing apparatus suitable for inputting handwritten characters or diagrams to a computer or a printer is disclosed. The apparatus includes an ultrasonic transmitter mounted on an input pen for transmitting ultrasonic waves, two ultrasonic receivers for receiving ultrasonic waves transmitted form the ultrasonic transmitter, and a distance calculating device for calculating distances between the input pen and the two ultrasonic receivers in order to determine coordinates representing a position of the input pen on the basis of the calculated distances. The apparatus of the invention can perform coordinate detection smoothly even when the input pen moves fast, and has reduced electric power consumption in the input pen to increase the life-span of a battery included in the input pen. Dibujos(15) Reclamaciones
DESCRIPTION OF THE PREFERRED EMBODUMENTS [0035]FIG. 1 is a schematically perspective view of an embodiment of the coordinate-capturing apparatus according to the invention, FIG. 2 is a top view of the apparatus, FIG. 3 is a view showing coordinates to be captured, FIG. 4 is a block diagram showing a circuit structure of the apparatus, and FIG. 5 is a time chart of various signals within the apparatus. [0036] As shown in FIGS. 1 and 2, the coordinate-capturing apparatus includes an input pen 1 for handwriting characters into a medium 20 such as a paper form, a main unit 11 which detects the coordinates of a locus of a tip portion of the input pen 1 when characters are written into the medium 20 by the input pen. The input pen 1 is sticklike. [0037] The main unit 11 is in the shape of a rectangular parallelepiped as a whole. The medium 20 and the main unit 11 are placed on a not illustrated plane, for example on a desktop. The medium 20 is placed on the plane such that its top side is in contact with or close to a side of the main unit 11. [0038] The main unit 11 captures coordinates of a position of the input pen 1 between the moment at which the input pen 1 comes in contact with the medium 20 and the moment at which the input pen 1 separates from the medium 20 at intervals of a predetermined sampling period. A state in which the input pen 1 is in contact with the medium 20 is referred to as �pen-down state�, and a state in which the input pen 1 is separate from the medium 20 is referred to as �pen-up state� hereinafter. Furthermore, one action between a pen-down and a subsequent pen-up is referred to as one �pen-stroke� or �stroke�. [0039] Characters written by the input pen 1 include not only alphanumeric characters, Chinese characters, and Japanese syllabaries but also symbols, diagrams, etc. [0040] The input pen 1 has a writing member 2 such as a core of a ballpoint pen for inking characters into the medium 20. The writing member is not limited to a core of a ballpoint pen. Any writing member can be used if it is long-life and easy to replace. The writing member is not indispensable for the apparatus of this embodiment. A sheet-type ultrasonic oscillator 3 of a polymeric material is wounded onto the surface of a jacket 1 a at the tip portion of the input pen 1 (in the vicinity of the writing member 2). The ultrasonic oscillator 3 is not limited to such a sheet type of a polymeric material. For example, a piezoelectric device such as PZT (PbZrO3�PbTiO3) can be used. An LED (light emitting diode) 4 is provided in the vicinity of the ultrasonic oscillator 3. [0041] A drive circuit 5 for driving the ultrasonic oscillator 3 and the LED 4, and a battery 6 are included in the input pen 1 (FIG. 2). The input pen 1 has a not illustrated switch for detecting a state in which the tip of the writing member 20 is pressed against the medium 20, that is, the pen-down state. The drive circuit 5 drives the ultrasonic oscillator 3 and the LED4 while the pen-down state is detected by this switch. [0042] A cylindrical-shaped member 12 a is provided at one end portion of the main unit 11 so as to project vertically therefrom, and a sheet-type ultrasonic receiver 13 a of a polymeric material is wound onto the side of this member 12 a. A cylindrical-shaped member 12 b is provided at the other end portion of the main unit 11 so as to project vertically therefrom, and a sheet-type ultrasonic receiver 13 b of a polymeric material is wound onto the side of this member 12 b. [0043] The ultrasonic receivers 13 a, 13 b are not limited to such a sheet-type of a polymeric material. Any piezoelectric device such as PZT (PbZrO3�PbTiO3) can be used. A light-receiving element 14 is provided between the ultrasonic receivers 13 a and 13 b. As shown in FIG. 3, the ultrasonic receivers 13 a, 13 b are located at the points R and S respectively on the straight line P, and separated from each other by the distance K. The medium 20 has a plane including the straight line P. The main unit 11 includes a signal processor 15 to which the ultrasonic receivers 13 a, 13 b, and the light-receiving element 14 are connected. [0044] The ultrasonic oscillator 3 and the drive circuit 5 of the pen 1 form an ultrasonic transmitter. The ultrasonic transmitter of this embodiment transmits a wave group (an ultrasonic pulse train) including p pulses having a frequency fS (p being 2 in FIG. 5) at a frequency fA=fS/h in the pen-down state. [0045] The LED 4 and the drive circuit 5 form a light signal transmitter. The light signal transmitter of this embodiment transmits a wave group (a light pulse train) including q pulses having a frequency fS (q being 2 in FIG. 5) at a frequency fB=fA/j (j being a positive integer greater than 2, for example, 10) in the pen-down state. [0046] The signal processor 15 has a clock pulse generating circuit 22, a light-receiving circuit 24, ultrasonic-receiving circuits 25 a, 25 b, counter circuits 26 a, 26 b, 28 a, 28 b, 30 a, 30 b, registers 27 a, 27 b, 29 a, 29 b, 32 a, 32 b, a fixed register 21, a coordinate-determination part 23, a variation-calculating circuits 31 a, 31 b, and adders 53 a and 53 b. [0047] The clock pulse generating circuit 22 generates clock pulses having a predetermined frequency FD (3 MHz, for example) continuously at least in the pen-down state. The light-receiving circuit 24 receives an output of the light-receiving element 14 and outputs a corresponding pulse signal (FIG. 5(E)). This signal is used as a start signal S. The ultrasonic-receiving circuits 25 a, 25 b receive outputs of the ultrasonic receivers 13 a, 13 b, and output corresponding ultrasonic-reception pulse signals GR, GL (FIG. 5(B) and (C)). [0048] The counter circuits 26 a, 26 b receive outputs of the clock pulse generating circuit 22, the light-receiving circuit 24, and the ultrasonic-receiving circuit 25 a, 25 b to measure the times elapsed between the moment at which the ultrasonic signal is emitted with the start signal S form the ultrasonic oscillator 3 and the moment at which it is received by the ultrasonic receivers 13 a, 13 b. [0049] The registers 27 a, 27 b hold the count values of the counter circuits 26 a, 26 b after completion of the counts (time clocking). Thereafter, the counter circuits 26 a and 26 b are reset to provide for the next counts. [0050] The counter circuits 28 a, 28 b receive outputs of the pulse generating circuit 22 and the ultrasonic-receiving circuits 25 a, 25 b, and count the number of the clock pulses generated between two successive pulses included in a pulse train generated at the ultrasonic-receiving circuits 25 a, 25 b. Thus, the time interval or pulse interval between two successive pulses can be determined. [0051] The registers 29 a, 29 b hold the count values of the counter circuits 28 a, 28 b after completion of the counts (time clocking). Thereafter, the counter circuits 28 a, 28 b are reset to provide for the next counts. [0052] The counter circuits 30 a, 30 b receive outputs of the pulse generating circuit 22 and the ultrasonic-receiving circuits 25 a, 25 b, and count the number of the clock pulses between generation of one pulse train and generation of the succeeding pulse train at the ultrasonic-receiving circuits 25 a, 25 b, that is, between reception of one pulse train and reception of the succeeding pulse train at the ultrasonic receivers 13 a, 13 b. Thus, the time interval between two successive pulse trains generated at the ultrasonic-receiving circuits 25 a, 25 b, that is, the time interval between two successive pulse trains received at the ultrasonic receivers 13 a, 13 b can be determined. [0053] The variation-calculating circuits 31 a, 31 b have multipliers 51 a, 51 b and subtracters 52 a, 52 b. The multipliers 51 a, 51 b multiply the output of the registers 29 a, 29 b by a constant h respectively. The outputs of the multipliers 51 a, 51 b represent a time interval between two successive ultrasonic pulse trains transmitted from the ultrasonic oscillator 3. The subtracters 52 a, 52 b subtract the outputs of the multipliers 51 a, 51 b from the outputs of the counter circuits 30 a, 30 b respectively. The outputs of the subtracters 52 a, 52 b, which are also the outputs of the variation-calculating circuits 31 a, 31 b, represent variations of the distances between the input pen 10 and the ultrasonic receivers 13 a, 13 b. [0054] The registers 32 a, 32 b hold the outputs (distance variations) of the variation-calculating circuits 31 a, 31 b respectively. [0055] The adders 53 a, 53 b add the values held in the registers 32 a, 32 b to the values held in the registers 27 a, 27 b respectively. The results of the additions are held in the registers 27 a, 27 b respectively. [0056] The fixed register 21 holds a value (NK) representing the distance between the ultrasonic receivers 13 a, 13 b. The coordinate-determination part 23 calculates coordinates (x-y coordinates, for example) representing a position of the input pen by trigonometry from the value held in the fixed register 21 and the values held in the registers 27 a, 27 b representing the distances between the input pen and the ultrasonic receivers 13 a, 13 b. The result of this calculation is transferred to an external unit (not shown) such as a memory or a computer, and stored there. [0057] This embodiment further includes a controller 16 for controlling the above-described components. [0058] The operation of this embodiment will now be explained referring to FIGS. 4, 5, etc. As a first step, the receiver-to-receiver distance NK (the number of the clock pulses) representing the distance K between the ultrasonic receivers is calculated as described below and stored in the fixed register 21. When the propagation speed of an ultrasonic wave in the air is v and the time required for the ultrasonic wave to travel the distance K is tk, the equation K=v�tK holds. When the frequency of the clock pulses generated by the clock pulse generating circuit 22 is FD, tK can be represented by the number of the clock pulses as tK=NK/FD, and accordingly, the equation NK=K�FD/v . . . (A1) holds. The coordinate-determining part 23 of the signal processor 15 sets up a rectangular coordinate system using the above NK calculated by the equation (A1), in which the straight line P makes an x axis in an x-y plane, the point R makes an origin point R(0, 0), and the coordinates of the point S are S (NK, 0) [0059] Here, FD=3 MHz, K=23.1 cm, and the NK is calculated at 2100 from the equation (A1) assuming that the ultrasonic propagation speed is 330 m/sec. This calculated NK is held in the fixed register 21. [0060] The principal of coordinate-detection with the input pen 10 will be explained below. At the start of a pen stroke, when the writing member 2 of the input pen 1 comes into contact with the medium 20 at the point Q1 shown in FIG. 3, the not illustrated switch turns on the drive circuit 5, whereby the ultrasonic oscillator 3 emits an ultrasonic signal US and the LED 4 emits a light-signal ES at the same time. This moment conforms to PEN-DOWN in FIG. 5. As shown in FIG. 5(A), the ultrasonic signal US is a wave group emitted at the frequency of fA=fS/h from the start of the pen-down or the pen stroke, each group ngm (m=1,2, . . . ,j) including p pulses of the frequency of fS. In this embodiment, p=2. The ultrasonic signal US is received by the ultrasonic receivers 13 a, 13 b, and converted into electric pulses in the ultrasonic-receiving circuits 25 a, 25 b respectively to generate ultrasonic-reception signals GR and GL. As shown in FIG. 5(D), the light signal ES is a wave group emitted at the frequency of fB=fA/j (j being an integer equal to or greater than 2) from the start of the pen-down or the pen stroke, each group ne including q pulses of the frequency fS. In this embodiment, q=2. The light signal ES is received by the light-receiving element 14, and processed in the light-receiving circuit 24 to generate the start signal S shown in FIG. 5(E). The time periods 1T1 R, 1T1 L between generation of a first start signal 1S and generation of first ultrasonic-reception signals 1G1 R , 1G1 L in response to a first wave group 1g1 of the ultrasonic signal US can be assumed to be propagation times required for the ultrasonic signal to travel from the ultrasonic oscillator 3 to the ultrasonic receivers 13 a, 13 b. The propagation times 1T1 R and 1T1 L are measured as the number of the clock pulses 1N1 R and 1N1 L having the frequency FD=3 MHz generated by the clock pulse generating circuit 22, and stored temporarily in the registers 27 a and 27 b respectively. The numbers 1N1 R and 1N1 L of the clock pulses translate into the distances 1L1 R, 1L1 L between the point Q1, and the ultrasonic receivers 13 a, 13 b respectively. It means that they are expressed as the same unit as the receiver-to-receiver distance NK. As seen from FIG. 3, three line segments corresponding to the distances 1N1 R, 1N1 L, and NK respectively form a triangle. Accordingly, the coordinate-determination part 23 can determine the position of the point Q1 as its coordinates Q1 (x1, y1) in the x-y coordinate system from the following equations (A2), (A3) by trigonometry. The determined position (coordinates) is stored in the memory (not shown), or transferred to the external unit such as a computer (not shown). [1 N 1 R]2 =[x 1]2 +[y 1]2 (A2) [1 N 1 L]2 =[N K −x 1]2 +[y 1]2 (A3) [0061] For example, if FD=3 MHz, and it has been detected that 1N1 R=1000, and 1N1 L=1700, it is determined that x1=600, and y1=800 since NK=2100. These determined values are stored in the memory (not shown), or transferred to the external unit such as a computer (not shown). [0062] As described above, the distances between the pen and the ultrasonic receivers 13 a, 13 b are determined from the times elapsed between the emission of the ultrasonic signal along with the light signal and the receptions of the ultrasonic signal by the ultrasonic receivers 13 a, 13 b. [0063] Subsequently, the counter circuits 28 a, 28 b count the numbers 1Nc1 R, 1Nc1 L of the clock pulses generated at the frequency FD by the clock pulse generating circuit 22 to measure periods 1Tc1 R, 1Tc1 L of the pulses of the ultrasonic-reception signals 1G1 R, 1G1 L having the frequency fS. These measurements are stored in the registers 29 a, 29 b and the counter circuits 28 a, 28 b are reset. Likewise, the counter circuits 30 a, 30 b count the numbers 1Ns1 R and 1Ns1L of the clock pulses generated at the frequency FD by the clock pulse generating circuit 22 to measure elapsed times 1Ts1 R, 1Ts1 L between rises of the ultrasonic-reception signals 1G1 R, 1G1 L and rises of second ultrasonic-reception signals 1G2 R, 1G2 L. At each of the risings of the second ultrasonic-reception signals 1G2 R, 1G2 L, the variation-calculating circuits 31 a, 31 b calculate the next variations 1D2 R, 1D2 L by the following equations. 1 D 2 R=1 Ns 1 R −h� 1 Nc 1 R (A4) 1 D 2 L=1 Ns 1 L −h� 1 Nc 1 L (A5) [0064] After the variations 1D2 R and 1D2 L are stored in the registers 32 a and 32 b, the registers 30 a and 30 b are reset. The variations 1D2 R, 1D2 L in the registers 32 a, 32 b are added to the last values stored in the registers 27 a, 27 b by the adders 53 a, 53 b, and the results of the addition are held in the registers 27 a, 27 b. Accordingly, the contents of the registers 27 a, 27 b become below-described 1N2 R, 1N2 L respectively. 1 N 2 R=1N1 R+1 D 2 R (A6) 1 N 2 L= 1 N 1 L+1 D 2 L (A7) [0065] The coordinate-determination part 23 determines the position of the point Q2 as its coordinates Q2 (x2, Y2) as in the case of determining the coordinates of the position of Q1 from the three values of 1N2 R, 1 N2 L and NK. The determined position is stored in the memory (not shown) or transferred to the external unit (not shown) such as a computer. In this embodiment, the frequency fS of the ultrasonic signal is about 50 KHz and the value of h is preset to 1,000 so that the wave group of the ultrasonic signal is transmitted at intervals of about 20 ms. Under such conditions, if it is found, when FD=3 MHz, that 1Nc1 R=59, 1Ns1 R=59,020, 1Nc1 L=59, 1Ns1 L=58,990, it is determined that 1D2 R=20, 1D2 L=−10, and subsequently it is determined that 1N2 R=1,020, 1N2 L=1,690. Accordingly, the coordinates of the position of the point Q2 can be determined as Q2 (618, 812) from the above-described three values including NK (=2,100). What is meant by the above determination will be explained below. The pen is at the point Q1 when the first wave group of the ultrasonic signal is emitted from the pen. The second wave group is emitted after a lapse of about 20 ms, which is equal to h�1Nc1 R=1000�59=59,000 in the number of the clock pulses of the frequency FD, from the transmission of the first wave group, and the pen moves to the point Q2 at that time. On the other hand, 1Ns1 R and 1Ns1 L represent, in the number of the clock pulses of the frequency FD, the times elapsed between the reception of the first wave group of the ultrasonic signal and the reception of the second wave group by the ultrasonic receivers. They vary depending on the distances between the point Q1 and the ultrasonic receivers and the distances between the point Q2 and the ultrasonic receivers. They decrease as the pen approaches the ultrasonic receivers and increase as the pen moves away therefrom. The variations 1D2 R, 1D2 L represent variations of the distances between the pen and the ultrasonic receivers when the pen moves from the point Q1 to the point Q2. The determination of 1D2 R=20 and 1D2 L =−10 indicates that the pen has moved away from the ultrasonic receiver 13 a and approached the ultrasonic receiver 13 b. [0066] When a third wave group arrives, the counter circuits 28 a, 28 b start counting again, and the counter circuits 30 a, 30 b are reset to start counting in order to calculate 1D3 R and 1D3 L by the following equations as in the case of calculating the coordinates of the point Q2. 1 D 3 R=1 Ns 2 R −h� 1 Nc 2 R (A8) 1 D 3 L= 1 Ns 2 L −h� 1 Nc 2 L (A9) [0067] Next, 1N3 R and 1N3 L are calculated by the following equations. 1 N 3 R=1 N 2 R+1 D 3 R (A10) 1 N 3 L=1 N 2 L+1 D 3 L (A11) [0068] Accordingly, a new position Q3 of the pen is determined as its coordinates Q3 (x3, y3) by the values of 1N3 R, 1N3 L and NK. Likewise, each time the wave group 1 G j arrives, 1Dj R and 1DJ L are calculated by the following equations. 1 D j R=1 Ns (j−1) R −h� 1 Nc (j−1) R (A12) 1 D j L=1 Ns (j−1) L −h� 1 Nc (j−1) L (A13) [0069] Subsequently, 1Nj R and 1NjL are calculated by the following equations. 1 N j R=1 N (j−1) R+1 D j R (A14) 1 N j L+1 N (j−1) L+1 D j L (A15) [0070] Thus, the coordinates Qj (xj,yj) of the point Qj are successively determined, and stored in the not illustrated memory, or transferred to the external unit such as a computer (not shown). [0071] When a second start signal 2S resulting from a second wave group 2e of the light signal is generated, all the counter circuits and all the registers except the fixed register 21 are reset. At that time, a wave group 1g(j+1) of the ultrasonic signal is being emitted. This wave group 1g(j+1) can be expressed as 2g1. The second start signal undergoes the same process as the first start signal. [0072] Thereafter, the above-described process is repeated until the pen is separate from the input plane and the not-illustrated switch of the pen is turned off. Then, the drive circuit 5 stops operating, and all the counter circuits and all the registers except the fixed register 21 are reset. Subsequently, a series of coordinates determined while the writing member 2 is in contact with the input plane is stored as data of one pen stroke in a memory or transferred to an external processing apparatus (not shown). [0073] When the writing member 2 comes into contact with the input plane again and the switch of the input pen is turned on, the above-described process is performed to determine a series of coordinates of a second pen stroke and transferred to the external processing apparatus. The same process is repeated for each pen stroke. [0074] As described above, in the first embodiment, a time period (pulse period) between receiving a pulse in a pulse train of the ultrasonic signal and receiving the succeeding pulse is clocked, and this clocked time period is multiplied by the ratio (a predetermined value: h) of the period of the ultrasonic pulse train to the pulse period to determined the time elapsed between emission of a pulse train of the ultrasonic signal and emission of the succeeding pulse train at the ultrasonic oscillator 3. [0075] In the first embodiment, the period of emission of the light signal is longer than the period of emission of the ultrasonic signal. The ratio j of the period of emission of the light signal to the period of emission of the ultrasonic signal is 2 or more. When the light signal and the ultrasonic signal are emitted at the same time, the distances between the pen and the ultrasonic receivers are determined on the basis of timings of receptions of these signals. On the other hand, when only the ultrasonic signal is emitted, distance variations are calculated and added to the last-determined distances to determine the current distances. Such a distance-update by calculation of distance variations brings about a buildup of an error, and therefore it is necessary to emit the light signal at times (at intervals longer than the ultrasonic signal emission period) to determine the distances directly. With such a process, it is possible to reduce the drain of the battery built in the pen since the frequency of the light signal emission is low. [0076] Furthermore, by emitting the ultrasonic signal at short intervals, it is possible to follow rapid movement of the pen and thereby provide data representing a smooth locus of the pen. [0077] The drain of the battery decrease as the ratio j increases. When the ratio j is infinite, that is, if the light signal is emitted only once at the start of a pen-down state, electric power consumption can be minimum. [0078] The second embodiment of the invention will now be described. The structure of the second embodiment is about the same as the first embodiment. FIG. 6 is a view explaining the difference between the first embodiment and the second embodiment. As shown in FIG. 6, a light-receiving circuit 34 is used instead of the light-receiving circuit 24 shown in FIG. 4, a counter circuit 35 is used instead of the counter circuits 28 a, 28 b shown in FIG. 4, and a register 35 is used instead of the registers 29 a, 29 b shown in FIG. 4. [0079] As described above, in the first embodiment, the periods nTcm R, nTcm L of the ultrasonic pulses of the frequency fS and the time elapsed between emission of an ultrasonic pulse train and emission of the succeeding ultrasonic pulse train at the ultrasonic oscillator 3 are determined from the pulses of the ultrasonic reception signals nGm R, nGm L. On the other hand, the second embodiment is arranged such that the light signal ES is processed by the light-receiving circuit 34 in FIG. 6 to generate a start signal (FIG. 5(E)) and a wave group nEc (FIG. 5(F)) corresponding to the light signal ES, in order to determine the period nTc of the ultrasonic pulses of the frequency fS from the wave group nEc. That is, in the second embodiment, the period nTc of the pulses having the frequency fS of the light signal ES (the time elapsed between receiving one pulse of the light signal and receiving the succeeding pulse) is measured by the counter circuit 35 as the number nNc of the clock pulses having the frequency FD generated by the clock pulse generating circuit 22, and is stored in the register 36. The output nNc of the register 36 is used as a substitute for nNcm R and nNcm L in the first embodiment. The output of the register 36 is multiplied by the factor h at the multipliers 51 a, 51 b to determine the time elapsed between emission of a ultrasonic pulse train and emission of the succeeding ultrasonic pulse train (the period of emission of the ultrasonic pulse train). [0080] Thereafter, the other processes that are the same as those in the first embodiment are carried out to determine the coordinates. [0081] As described above, in the second embodiment, the time elapsed between receiving an ultrasonic pulse train and receiving the succeeding ultrasonic pulse train is determined by multiplying the time between receiving a pulse of the light signal and receiving the succeeding pulse of the light signal by the factor h. [0082] Although reference has been made to the cases where p=2 and q=2, it is obvious that the first embodiment allows p≧2 and q≧1, and the second embodiment allows p≧1 and q≧2. The factor h is preset such that h/fS, which is a coordinate-sampling interval, becomes a desired value that should be larger than the maximum propagation time required for the ultrasonic signal travels from the pen on the input plane to the ultrasonic receivers. [0083] The third embodiment will now be described. In this embodiment, nNcm R and nNcm L measured in the first embodiment and nNc measured in the second embodiment are not used, but [h/fS]�FD calculated beforehand is used instead of h�nNcm R and h�nNcm L, or h�nNc. The third embodiment is a modification of the first embodiment shown in FIG. 4, in which the counter circuits 28 a, 28 b, the registers 29 a, 29 b, and the multipliers 51 a, 51 b are removed, and the output of a fixed register 40 storing the value of [h/fS]�FD is supplied to the subtracters 52 a, 52 b as shown in FIG. 7. It is obvious that the third embodiment allows p≧1 and q≧1. The third embodiment can be used when the frequency of emission of the ultrasonic wave group (fS/h) is constant. If the frequency varies by a large amount, its position-detection accuracy is deteriorated. If the frequency variation is small, it is possible to reduce power consumption in the pen and to simplify the circuit structure of its receiver side without deteriorating the accuracy. [0084] In the above-described first to third embodiments, the ultrasonic signal is emitted intermittently, whereas, in the below-described fourth to seventh embodiments, the ultrasonic signal is emitted continuously. [0085]FIG. 8 shows a circuit structure of the fourth embodiment. The structure of the fourth embodiment is about the same as the first embodiment. The reference numerals in FIG. 8 identical to those in FIG. 4 represent the same or corresponding elements. [0086] In this embodiment, the drive circuit 5 is replaced by a drive circuit 105 that causes the ultrasonic oscillator 3 to emit the ultrasonic signal having the frequency fS continuously during the pen-down state. On the other hand, the drive circuit 105 causes the LED 4 to emit the light signal having a single pulse only once at the start of the pen-down state. This light signal serves as a start signal ER. [0087] The counter circuits 126 a, 126 b receive the outputs of the clock pulse generating circuit 22, the light-receiving circuit 24 and the ultrasonic-receiving circuits 25 a, 25 b, and count the clock pulses from the moment of generation of the start signal ER and the moment of generation of ultrasonic-reception signals. Thus, the times elapsed between the moment at which the ultrasonic signal is emitted from the ultrasonic oscillator 3 along with the start signal ER and the moment at which it is received by the ultrasonic receivers 13 a, 13 b can be measured. [0088] The registers 127 a, 127 b hold the counts of the counter circuits 126 a, 126 b after completion of the counts (time measurement). [0089] The counter circuits 128 a, 128 b receive the outputs of the ultrasonic-receiving circuits 25 a, 25 b, and count the pulses of the ultrasonic-reception signals respectively. The counter circuits 129 a, 129 b receive the outputs of the clock pulse generating circuit 22 and the ultrasonic-receiving circuits 125 a, 125 b, and count the clock pulses respectively. As described later, the outputs of the counter circuits 128 a, 128 b and the counter circuits 129 a, 129 b, which are the count values for the same time period, are used to calculate distance variations in variation-calculating circuits 131 a, 131 b. The counts of the counter circuits 128 a, 128 b for a certain time period represent a time interval between emission of a certain part of the ultrasonic signal (m-th pulse, for example) and emission of a later part of this signal ((m+n) th pulse, for example) at the ultrasonic oscillator 3. The counts of the counter circuits 129 a, 129 b for the same time period represent the times elapsed until the ultrasonic receivers 13 a, 13 b receive the (m+n) th pulse after receiving the m-th pulse respectively. However, since the counter circuits 129 a, 129 b count the clock pulses of the frequency FD, while the counter circuits 128 a, 128 b count the pulses of the frequency fS, the registers 130 a, 130 b hold the counts of the counter circuits 129 a, 129 b after completion of the time measurement. Thereafter, the counter circuits 129 a, 129 b are reset (their counts are reset to the initial value 0) to provide for the next count. [0090] The variation-calculating circuits 131 a, 131 b have multipliers 134 a, 134 b and subtracters 135 a, 135 b. [0091] The multipliers 134 a, 134 b multiply the outputs of the counter circuits 128 a, 1278 b by the constant FD/fS, respectively. It is for taking account of the frequency difference between the pulses counted by the counter circuits 128 a, 128 b and the pulses counted by the counter circuits 129 a, 129 b. Thus, the outputs of the multipliers 134 a, 134 b represent the time interval between emissions at the ultrasonic oscillator 3 in the same unit in which the elapsed time between receptions at the ultrasonic receivers 13 a, 13 b is represented. [0092] The subtracters 135 a, 135 b subtract the outputs of the registers 130 a, 130 b from the outputs of the multipliers 134 a, 134 b, respectively. The outputs of the subtracters 135 a, 135 b, which are the outputs of the variation-calculating circuits 131 a, 131 b, represent variations of the distances from the input pen to the ultrasonic receivers 13 a, 13 b. [0093] The registers 132 a, 132 b hold the outputs (distance variations) of the variation-calculating circuits 131 a, 131 b. [0094] A variation-comparison circuit 133 determines whether the distance variations held in the registers 132 a, 132 b satisfy an expression (B6) or (B7) described later. If the variation-comparison circuit 133 determines that the expression (B6) or (B7) is satisfied, the values held in the registers 132 a, 132 b are added to the values held in the registers 127 a, 127 b. The results of the addition are held in the registers 127 a, 127 b. [0095] The coordinate-determination part 23 calculates coordinates (for example, x-y coordinates) representing the position of the input pen by trigonometry from the value held in the fixed register 21, and the values representing the distances from the input pen to the ultrasonic receivers 13 a, 13 b held in the registers 127 a, 127 b. The result of the calculation is transferred to a not-illustrated memory or an external unit such as a computer, and held there. [0096] The fourth embodiment will now be described with reference to FIG. 9 and FIG. 10. When the writing member 2 of the pen 1 comes into contact with the input plane 20 at the point Q0 as shown in FIG. 9, the not-illustrated switch of the input pen is turned on to cause the ultrasonic oscillator 3 to emit the ultrasonic signal US, and cause the LED 4 to emit the light signal ES at the same time through the drive circuit 105 shown in FIG. 8 (PEN-DOWN 1 in FIG. 10). As shown in FIG. 10(C), the ultrasonic signal US is oscillating at the frequency fS while the writing member 2 is in contact with the input plane, that is, during the pen stroke. This ultrasonic signal US is received by the ultrasonic receivers 13 a, 13 b, and converted into ultrasonic-reception signals UR, UL (electric pulse signals) by the ultrasonic-receiving circuits 25 a, 25 b. The light signal ES, which is a wave group including q pulses having the frequency p times (p being a positive integer) higher than the oscillation frequency fS of the ultrasonic oscillator, is emitted only once at the start of each pen stroke. FIG. 10(A) shows a case where p=1 and q=1. The light signal ES is received by the light-receiving element 14, and converted into a start signal ER (electric pulse signal) indicating the start of the pen down state by the light-receiving circuit 24. The times 1tR0, 1tL0 between generation of the start signal ER and generation of the ultrasonic-reception signals UR, UL can be regarded as propagation times required for the ultrasonic signal to travel from the ultrasonic oscillator 3 to the ultrasonic receivers 13 a, 13 b, since the propagation time of the light signal is as small as negligible. The propagation times 1tR0, 1tL0 are clocked by the counter circuits 126 a, 126 b as the numbers N0 R, N0 L of the clock pulses having the frequency FD=3 MHz generated by the clock pulse generating circuit 22. The numbers N0 R, N0 L of the clock pulses, which translate into the distances L0 R, L0 L between the point Q0 and the ultrasonic receivers 13 a, 13 b, are temporarily stored as equivalents of the distances in the registers 127 a, 27 b. The above equivalents N0 R, N0 L are expressed in the same unit with NK that is the equivalent of the distance between the ultrasonic receivers. As seen from FIG. 9, three line-segments connecting the above N0 R, N0 L and NK form a triangle. The coordinate-determination part 23 determines the position of the point Q0 as its coordinates Q0 (x0,y0) in the x-y coordinate system in accordance with the following equations (B2), (B3) by trigonometry. The coordinates determined are stored in a not-illustrated memory or transferred to an external unit such as a computer. [N 0 R]2=[x 0]2 +[y 0]2 (B2) [N 0 L]2=[N K −x 0]2 +[y 0]2 (B3) [0097] If N0 R=1000 and N0 L=1700 when FD=3 MHz, x0=600 and y0=800 are calculated from NK=2100, and are stored in a not illustrated memory or transferred to a not illustrated external unit such as a computer. [0098] The switch of the pen remains closed while the input pen 1 is in contact with the input plane 20, that is, during the pen stroke. Accordingly, the oscillation of the ultrasonic signal US continues and the pulses of the ultrasonic reception signals UR, UL are delivered continuously. The counter circuits 128 a, 128 b continue to count the numbers nR, nL of these pulses, and the counter circuits 129 a, 129 b continue to count the numbers TR, TL of the clock pulses generated by the clock pulse generating circuit 22 at the frequency FD as equivalents of the times tR, tL elapsed from the starts of the ultrasonic reception signals UR, UL respectively. The numbers TR, TL of the pulses in the counter circuits 129 a, 129 b when the counter circuits 128 a, 128 b count up to n1 R, n1 L respectively, are successively stored in the registers 130 a, 130 b as TR1 (n1 R) and TL1 (n1 L). Furthermore, their respective variations DR1 (n1R), DL1 (n1 L) are calculated every moment by the variation-calculating circuits 131 a, 131 b according to the following equations (B4) and (B5) and successively stored in the registers 132 a, 132 b respectively. DR 1 ( n 1 R) =TR 1 ( n 1 R) −[n 1 R−1]�F D / f S (B4) DL 1 ( n 1 L ) =TL 1 ( n 1 L) −[n 1 L−1]�F D /f S (B5) [0099] The variation-comparison circuit 133 compares the absolute values of the variations DR1 (n1 R), DL1 (n1 L) with a predetermined value d to determine whether the following inequalities (B6), (B7) are satisfied. |DR 1 ( n 1 R) |≧d, |DL 1 ( n 1 L) |<d (n1 L=1, 2, . . . n 1 R) (B6) |DL 1 ( n 1 L) |≧d, |DR 1 ( n 1 R) |<d (n1 R=1, 2, . . . n 1 L) (B7) [0100] If either of the inequalities (B6), (B7) is satisfied when an n1-th pulse of the ultrasonic signal US emitted from the pen situated at the position Q1, which had been moved from the Q0, has arrived at the ultrasonic receivers, the variations DR1 (n1 ), DL1 (n1 ) corresponding to the n1-th pulse are output from the registers 132 a, 132 b as the first variations DR1, DL1 and added to the values stored in the registers 127 a, 127 b by the adders 136 a, 136 b. The results of the addition are held in the registers 127 a, 127 b. Thus, the values stored in the registers 127 a, 127 b become distance-equivalent values N1 R, N1 L expressed in the following equations (B8) and (B9). N 1 R =N 0 R +DR 1 (B8) N 1 L =N 0 L +DL 1 (B9) [0101] The coordinate-determination part 23 determines the coordinates Q1 (x1,y1) of the point Q1 from the values of N1 R, N1 L and NK, and stores them in the not illustrated memory or transfers them to the not illustrated external unit such as a computer. [0102] The inequalities (B6), (B7) are satisfied when the distance variation exceeds the value of d. As described above, each time the distance variation exceeds the predetermined value, this variation is added to the distance value (the value stored in the register 127 a or 127 b) determined by the preceding calculation, and the result of the addition is stored in the register 127 a or 127 b as a new distance value. The coordinate-determination part 23 determines new coordinates based on this new distance value. [0103] The calculation of the distance variation in the variation-calculating circuit 131 a or 131 b can be performed each time the number of the pulses counted by the counter circuit 128 a or 128 b reaches a predetermined number, or each time the number of the pulses counted by the counter circuit 129 a or 129 b reaches a predetermined number. [0104]FIG. 10 shows a case where DR1 111 becomes −18 when n1 R=111 and thereby the inequality (B6) (|DR1 (n1 R)|≧15) is first satisfied under the conditions of the oscillation frequency of the ultrasonic signal being 50 KHz and the value d being 15. Subsequently, when n1 L=101, DL1 101 becomes 20 to satisfy the inequality (B7). However, the inequality (B6) is not satisfied since n1 R becomes 150 at that moment. Therefore, the value of DL1 101 is added to the value in the register 127 b as DL1=20, and n1 L=101=n1. On the other hand, if the value of DR1 101 stored in the register 132 a is −10 at that moment, the value of DR1 101 is added to the value stored in the register 127 a as DR1=−10. In consequence, the values of N1 R and N1 L held in the registers 127 a and 127 b are changed as N1 R=1010, N1 L=1680 respectively according to the equations (B8) and (B9). The coordinate-determination part 23 determines the coordinates of the point Q1 as Q1 (621, 797) from the three values of N1 R=1010, N1 L=1680 and NK=2100. What is meant by the above determination will be explained below. When the ultrasonic oscillator 3 emits the first pulse, the writing member 2 of the pen 1 is at the point Q0. The pen is moving, and therefore the writing member is at the point Q1 when n1 1=101, that is, 100�1/fS after the emission of the first pulse. In other words, the writing member 2 is at the point Q1 after 6000 (100�FD/fS=100�3000/50) clock pulses of the frequency FD are generated when the 101st ultrasonic pulse is just emitted. At that moment, TR1 101 and TL1 101 represent, in the numbers of the clock pulses having the frequency FD, the times between reception of the first ultrasonic pulse and reception of the 101st ultrasonic pulse by the ultrasonic receivers 13 a, 13 b that are equivalents of the propagation times required for the ultrasonic signal travel from the point Q1 to the ultrasonic receivers 13 a, 13 b. Accordingly, the variations DR1 101, DL1 101 represent a travel of the writing member 2 with respect to the ultrasonic receivers 13 a, 13 b corresponding to the movement of the writing member from the point Q0 to the pint Q1. What is meant by DR1 101=−10 and DL1 101=20 is that the pen is moving closer to the ultrasonic receiver 13 a and moving away from the ultrasonic receiver 13 b. [0105] When either of the inequalities (B6), (B7) is satisfied, the counts of the counter circuits 128 a, 128 b are reduced by [n1−1] to become n2 R and n2 L respectively to provide for the next counts. Furthermore, the count of the counter circuit 129 a is reduced by the value of TR1 (n1 1) held in the register 130 a to become TR2 (n2 R), and the count of the counter circuit 129 b is reduced by the value of TL1 (n1 1) held in the register 130 b to become TL2 (n2 L) to provide for the next counts. The register 130 a holding the values corresponding to TR1 1 to TR1 (n1 ), and the register 130 b holding the values corresponding to TL1 1 to TL1 (n1 ) are reset to provide for storing new values as TR2 (n2 R) and TL2 (n2 L) respectively. Likewise, the register 132 a holding the values corresponding to DR1 1 to DR1 (n1 ), and the register 132 b holding the values corresponding to DL1 1 to DL1 (n1 ) are reset to provide for storing new values as DR2 (n2 R) and DL2 (n2 L) respectively. A new variation DR2 (n2 R) or DL2 (n2 L) is calculated from TR2 (n2 R) or TL2 (n2 L) held in the register 130 a or 130 b which has been just reset and n2 R or n2 L on the basis of the following equation (B10) or (B11) which is equivalent of the equation (B4) or (B5). The register 132 a or 132 b holding data for more than n1 pulses at the time of above reset is rewritten to have the above new variation to provide for the next operation. DR 2 ( n 2 R) =TR 2 ( n 2 R) −[n 2 R) ]�F D /f S (B10) DL 2 ( n 2 R) =TL2( n 2 L) −[n 2 L−1]�F D /f S (B11) [0106] In the case of FIG. 10 where the inequality (B7) is satisfied when n1=101, the count of the counter circuit 128 a is 150, DL1 101 held in the register 132 b is 20, and DR1 101 held in the register 132 a is −10 when the count of the counter circuit 128 b reaches 101. At that moment, the variation-calculating circuits 131 a, 131 b output DR1=−10 and DL1=20, so that the count of the counter circuit 128 a is reduced by [101−1]=100 to change from 150 to n2 R=50, and the count of the counter circuit 128 b is reduced by 100 to change from 101 to n2 L=1. New counts start from this state. The count of the counter circuit 129 b is TL2 1=0 since TL1 101 (6000+20=6020)−TL1 101=0, and the count of the counter circuit 129 a is, if TR1 150 has reached 8925 at that moment, TR2 50=2935 since TR150(8925)−TR101(6000−10=5990)=2935. New counts start from this state. The register 130 b holds TL21=0, and the register 132 b holds DL21=0 under such a reset state. On the other hand, the values corresponding to TR1 101 to TR1 150 held in the register 130 a at that moment are reduced by TR1 101=5990 respectively and are left in the register 130 a as the values corresponding to TR2 1 to TR2 50. The register 132 a holding the values corresponding to DR1 101 to DR1 150 at that moment are rewritten to hold the values of DR2 1 to DR2 50 that are calculated from the values of TR2 1 to TR2 50 currently held in the register 130 a. For example, DR2 50=TR2 50−49�60=2935−2940=−5. [0107] The moment at which the n1-th pulse of the ultrasonic signal is emitted is used as a reference time for carrying out a second sampling. That is, a process similar to the above-described process for determining the coordinates of the point Q1 is carried out regarding that a first pulse for the second sampling is emitted at this moment. If the pen is at the position Q2 when an n2-th pulse of the ultrasonic signal is emitted after the new reference time, and the arrival of this n2-th pulse at the ultrasonic receiver satisfies one of the following inequalities (B12) and (B13) that are the equivalents of the inequalities (B6) and (B7), |DR 2 ( n 2 R) |≧d, |DL 2 ( n 2 L) |<d (n2 L=1, 2, . . . n 2 R) (B12) |DL 2 ( n 2 L)| ≧d, |DR 2 ( n 2 R)| <d (n2 R=1, 2, . . . n 2 L) (B13) [0108] The variations DR2 (n2) and DL2 (n2 ) with respect to the n2-th pulse are output from the variation-calculating circuits 131 a, 131 b as variations DR2, DL2, and N2 R and N2 L are determined according to the following equations (B14) and (B15) that are the equivalents of the equations (B8) and (B9). N 2 R =N 1 R +DR 2 (B14) N2 L =N 1 L +DL 2 (B15) [0109] The coordinate-determination part 23 determines the coordinates Q2 (x2,y2) of the point Q2 from the N2 R, N2 L and NK, and stores them in the not illustrated memory or transfers them into the not illustrated external unit such as a computer. [0110] By carrying out an m-th sampling, DRm (nm R) and DLm (nm L) are calculated according to the following equations (B16) and (B17). DR m ( n m R) =TR m ( n m R) −[n m R−1]�F D /f S (B16) DL m ( n m L) =TL m ( n m L) −[n m L−1]�F D /f S (B17) [0111] Subsequently, when the following inequalities (B18) and (B19) are satisfied, |DR m ( n m R) |≧d, |DL m ( n m L) |<d (nm L=1, 2, . . . n R) (B18) |DL m ( n m L) |≧d, |DR m ( n m R) |<d (nm R=1, 2, . . . n L) (B19) [0112] Nm R and Nm L are determined according to the following equations (B20) and (B21) as DRm (nm R)=DR m, DLm (nm L)=DLm L. N m R =N (m−1) R +DR m (B20) N m L =N (m−1) L +DL m (B21) [0113] Then, the coordinates Qm (xm,ym) of the point Qm are determined, and stored in the not illustrated memory or transferred to the not illustrated external unit such as a computer. [0114] Thereafter, when the writing member 2 separates from the input plane 20, the switch (not illustrated) of the pen 1 is turned off, and thereby the oscillation of the ultrasonic oscillator 3 ceases (PEN-UP 1 in FIG. 10). In consequence, the counter circuits 126 a, 126 b, 128 a, 128 b, 129 a, and 129 b, and the registers 127 a, 127 b, 130 a, 130 b, 132 a, and 132 b are reset, and then a series of coordinates determined while the writing member 2 is in contact with the input plane 20 is stored in the memory or transferred to the external unit as stroke data. [0115] When the writing member 2 again comes into contact with the input plane and the switch of the pen 1 is turned on, measurement of the propagation times 2tR0 and 2tL0 is started for determining the initial position of the pen in the second pen stroke (PEN-DOWN 2 in FIG. 10). By carrying out the above-described processes, a series of coordinates for the second pen stroke is determined and stored in the memory or transferred to the external unit. [0116] In the above described embodiment, p=1 and q=1, however, it is obvious that p and q can be any positive integer. [0117] The fourth embodiment described above can perform coordinate-determination smoothly even when the pen is moving fast, since the ultrasonic oscillator oscillates continuously during a pen stroke and timing of coordinate-sampling is determined based on the amount of the travel of the pen. [0118] However, in the fourth embodiment, when determining coordinates of points after Q1 in accordance with appropriate expressions such as equations (B16) and (B17), since [FD/fS] used in the multipliers 134 a, 134 b is a predetermined constant, an error may occur in the calculation due to pen-to-pen variation in the oscillation frequency fS. The fifth embodiment described below aims at solving this problem. [0119] The fifth embodiment will now be described. The structure of the fifth embodiment is the same as the fourth embodiment as a whole. The difference is in the circuit structures of variation determination circuits 140 a, 140 b. The variation-calculating circuits 140 a, 140 b replacing the variation-calculating circuits 131 a, 131 b, have reference-time detecting circuits 141 a, 141 b, registers 142 a, 142 b, multipliers 143 a, 143 b, and subtracters 144 a, 144 b. [0120] The reference-time detecting circuits 141 a, 141 b receive the output (clock pulses) of the clock pulse generating circuit 22 and the outputs of the ultrasonic-receiving circuits 25 a, 25 b to determine the ratio FD/fS by counting the clock pulses over one or more cycles of the ultrasonic signal. For example, if the count of the clock pulses for n cycles of the ultrasonic signal is m, FD/fS equals to m/n. To be more specific, in the fourth embodiment, the clock pulses generated by the clock pulse generating circuit 22 is counted over the period tcR or tcL of the first cycle of the ultrasonic reception signal UR or UL shown in FIG. 10(D) or (E) for each pen stroke, and the count NUR or NUL is determined as FD/fS. [0121] The registers 142 a, 42 b hold the ratio FD/fS determined by the reference-time detecting circuits 141 a, 141 b. [0122] The multipliers 143 a, 143 b multiply the outputs of the registers 142 a, 142 b by the outputs of the counter circuits 128 a, 128 b respectively. [0123] The subtracters 144 a, 144 b subtract the outputs of the multipliers 143 a, 143 b from the outputs of the registers 130 a, 130 b respectively. [0124] The multipliers 143 a, 143 b, and the subtracters 144 a, 144 b are used to calculate distance variations D′Rm(nm R) and D′Lm(nm L) in accordance with the following equations (B22), (B23). D′R m ( n m R) =TR m ( n m R) −[n m R−1]�N UR (B22) D′L m(n m L)=TL m(n m L)−[n m L−1]�N UL (B23) [0125] The distance variations D′Rm(nm R) and D′Lm(nm L) are stored in the registers 132 a, 132 b. The other processes carried out in the fifth embodiment are the same as those carried out in the fourth embodiment. [0126] As described above, the fifth embodiment differs from the fourth embodiment in that [FD/fS] is replaced by NUR or NUL in the equations (B16), (B17) [0127] In the fifth embodiment, since FD/fS is determined by actually measuring the oscillation frequency of the ultrasonic oscillator of the pen by counting the clock pulses, it is possible to eliminate errors due to pen-to-pen variation in the oscillation frequency fS. [0128] The sixth embodiment where p=3 and q=2 will be described below. The structure of the sixth embodiment is about the same as that of the fourth embodiment. The difference is in a different light-receiving circuit 150 and a variation-calculating circuit 151 shown in FIG. 12. [0129] The light-receiving circuit 150 replacing the light-receiving circuit 24 in the fourth embodiment includes a pulse-generating circuit 152 and a start signal generator 153. The pulse-generating circuit 152 converts a light signal EP (FIG. 13(B)) into a pulse signal as a light reception signal EC (FIG. 13(C)). [0130] The start signal generator 153 generates, in response to the output of the pulse-generating circuit 152, a start signal ER which is an equivalent of the start signal ER in the fourth embodiment. [0131] The variation-calculating circuit 151, which replaces the variation-calculating circuits 140 a, 140 b, includes a reference-time detecting circuit 154, a register 155, multipliers 143 a, 143 b, and subtracters 144 a, 144 b. [0132] The reference-time detecting circuit 154 measures a period tS of a first cycle of the light-reception signal EC by counting the number NS of the clock pulses generated by the clock pulse generating circuit 22 at the frequency FD. The register 155 holds the result of the measurement. [0133] The multipliers 143 a, 143 b, and the subtracters 144 a, 144 b are the same as those shown in FIG. 11. But one input of each of the multipliers 143 a, 143 b is connected to the register 155. FIG. 13(A) shows a waveform of the ultrasonic signal US that is the same as the one in the fourth embodiment. [0134] The multipliers 143 a, 143 b, and the subtracters 144 a, 144 b are used to calculate distance variations D″Rm (nm R), and D″Lm (nm L) according to the following equations B(24), B(25). D″R m ( n m R) =TR m ( n m R) −[n m R−1]�p(=3)�N S (B24) D″L m ( n m L) =TL m ( n m L) −[n m L−1]�p(=3)�N S (B25) [0135] These calculated variations D″Rm (nm R) and D″Lm (nm L) are stored in the registers 132 a, 132 b. The other processes are the same processes as those in the fourth embodiment. That is, [FD/fS] in the fourth embodiment is replaced by the above-described NS. It is needless to say that the processes for determining coordinates used in the fourth embodiment can be used in the sixth embodiment as well, and q may be greater than two. [0136] As described above, the sixth embodiment is arranged to count the clock pulses for one period of the light signal and obtain the product of the value of this count and the ratio of the period of the light signal to that of the ultrasonic signal as an equivalent of [FD/fS]. [0137] The seventh embodiment of the invention where p=1 and q is infinite, that is, a case of continuous emission will now be described. [0138] The structure of the seventh embodiment is about the same as that of the sixth embodiment. The difference is in a variation-calculating circuit shown in FIG. 14. FIG. 15 shows signal waveforms in the seventh embodiment. [0139] This variation-calculating circuit 160 has a counter circuit 161, a register 162, and multipliers 143 a, 143 b. [0140] The counter circuit 161 measures a time period between a rise of a first pulse and a rise of an n-th pulse of the light-reception signal EC (FIG. 15(c)) corresponding to the light signal EP (FIG. 15(B)) in an m-th (m=1,2,3, . . . ) sampling by counting the number of the clock pulses having the frequency FD as TVm (nm). The results of this measurement are successively stored in the register 162. The subtracters 144 a, 144 b subtract the output of the register 162 from the outputs of the registers 128 a, 128 b respectively. That is, the distance variations D′″Rm (nm R) and D′″Lm (nm L) are calculated according to the following equations (B26), (B27). D′″R m ( n m R) =TR m ( n m R) −TV m ( n m ) (B26) D′″L m ( n m L) =TL m ( n m L) −TV m ( n m ) (B27) [0141] Thus caslculated D′″Rm (nm R) and D′″Lm (nmL) are stored in the registers 132 a, 132 b. The other processes are the same as those in the fourth embodiment. [0142] As described above, in the seventh embodiment, the light signal is emitted continuously in synchronization with the ultrasonic signal and the pulses of the light signal received by the light-receiving element are counted to measure an elapsed time between emission of the m-th pulse and emission of the (m+n)-th pulse of the ultrasonic signal at the ultrasonic oscillator. [0143] The sixth and the seventh embodiments are arranged to measure the frequency of the light signal emitted from the pen side in synchronization with the ultrasonic signal at the receiving side, and to calculate the distance variation based on the measured frequency. Therefore, they can determine coordinates accurately without being affected by the pen-to-pen variation in the emitting frequency. [0144] The eighth embodiment, which is a variant of the fourth to seventh embodiments, will now be described. [0145] In the fourth to seventh embodiments, the timing of coordinate acquisition (sampling timing) after Q1 is determined to be an instant at which the inequality (B18) or (B19) is satisfied. However, it is also possible to initiate a sampling each time the number of the counted pulses of the continuously oscillating ultrasonic signal from the pen reaches a predetermined value. Accordingly, in this embodiment, the successive calculations of variations in the fourth to seventh embodiments are not performed, but calculations of D′″Rm and D′″Lm are performed instead according to the following equations (B28), (B29). D′″R m =TR m −J (B28) D′″L m =TL m −J (B29) [0146] where [0147] Cm is a variable coefficient; [0148] J=Cm�FD/fS . . . (when applied to the fourth embodiment); [0149] J=Cm�NUX (X:R or L) . . . (when applied to the fifth embodiment) [0150] J=Cm�NS . . . (when applied to the sixth embodiment); and [0151] J=TVm c m ) . . . (when applied to the seventh embodiment). [0152] Here, D′″Rm and D′″Lm are the same as DRm and DLm within the equations (B20) and (B21) used in the fourth to seventh embodiments, and Cm is set according to the followings. At the start of the stroke, that is, at the time of sampling Q1, a fixed value C1 is used. For subsequent samplings, Cm is determined by comparing the absolute values of the last calculated D′″Rm and D′″Lm with the predetermined values dL and dS (dL>dS). To be more specific, Cm is determined from an arithmetic progression Cn prepared beforehand to satisfy the followings. When |D′″R m |≧d L or |D′″L m |≧d L (B30), C (m+1) <C m (B31). When |D′″R m |≦d S or |D′″L m |≦d S (B32), C (m+1) >C m (B33). [0153] When the inequalities (B30) and (B32) are not satisfied, C (m+1) =C m (B34). [0154] The ninth embodiment, which is a variant of the fourth to eighth embodiments, will now be described. The fourth to eighth embodiments are described as �2-ultrasonic-wave+electromagnetic-wave type� system using a pen having an ultrasonic oscillator and a light emitter, however, they can be a �3-ultrasonic-wave type� system. [0155] In this case, at least three ultrasonic receivers X, Y, Z are disposed on the same plane to receive the ultrasonic signal from the pen as shown in FIG. 16. When the pen comes into contact with the plane at the point G0, the ultrasonic oscillator of the pen starts to emit the ultrasonic signal continuously. Then a hyperbolic curve w1 in the x′-y′ coordinate system including the above X, Y, Z is determined from the difference of timings of receptions between the receivers X and Y, and likewise, another hyperbolic curve w2 in the x′-y′ coordinate system is determined from the difference of timings of receptions between the receivers Y and Z. The position of the point G0 is determined as the point of intersection of these hyperbolic curves w1 and w2. Subsequently, the distances Ix and Iy between the point G0 thus determined and the receivers X, Z are determined. Thereafter the same processes as those in the fourth, fifth or eighth embodiment is performed for determining coordinates of the position Gm of the pen. [0156] The tenth embodiment where the distance between the receivers 13 a and 13 b is made variable to adapt to input mediums of various widths will now be described. [0157] The structure of this embodiment is about the same as the first embodiment. The difference is in that the ultrasonic receiver 13 b is mounted so at to be position-adjustable as shown in FIG. 17, and the signal processor 15 is modified accordingly as shown in FIG. 18. [0158] The signal processor 15 includes a coordinate-determination circuit 223 corresponding to the coordinate-determination part 23 of FIG. 8, a light-receiving circuit 224 corresponding to the light-receiving circuit 24 of FIG. 8, ultrasonic-receiving circuits 225 a, 225 b corresponding to the ultrasonic-receiving circuits 25 a, 25 b of FIG. 8, counter circuits 226 a, 226 b corresponding to the counter circuits 126 a, 126 b of FIG. 8. The signal processor 15 further includes a distance-measuring device 220 for measuring a variable distance K′ between the ultrasonic receivers 13 a and 13 b, a coordinate-conversion circuit 222, and a data storage 228 for storing coordinates after coordinate-conversion. [0159] At the time of writing into the form 20, the position of the receiver 13 b is adjusted such that the distance K′ is about the same as the length of the side AB of the form which is in contact with or close to the main unit 11. The distance K′ measured by the distance-measuring device 220 is input to the coordinate-determination circuit 223 to be used as an equivalent of NK representing the distance between the receivers 13 a and 13 b. Then the points C, D at each end portion of the sides AB are pressed in turn by the pen to acquire x-y coordinates of the points C, D. Then a new x′-y′ coordinate system whose origin point is the point C and whose x′ axis is a straight line passing through the points C, D is established. After the process for sampling and acquiring x-y coordinates as described in the first embodiment is performed, the coordinate-conversion circuit 222 converts the x-y coordinates into x′-y′ coordinates and stores them in the data storage 228. [0160] With the tenth embodiment, it is possible to handle forms of various sizes. Especially, when a form of small size is used, since resolution in position determination is increased, small characters can be recognized accurately. [0161] Although reference has been made to the cases where a light signal is emitted along with an ultrasonic signal from the pen as described in the first to eighth embodiments, electromagnetic waves for wireless transmission can be used instead of the light signal. The present invention is also applicable to a case where a timing signal is transmitted through a cable from the pen to the signal processor of the main unit. The coordinate-capturing apparatus of the present invention is not limited to the above described ultrasonic aerial-propagation type. It may be an ultrasonic in-medium propagation (surface acoustic wave) type. Furthermore, although it has been described that the timing signal and the ultrasonic signal are emitted only during the pen-down state, the present invention is applicable to a case where they are emitted all the time. [0162] The above explained preferred embodiments are exemplary of the invention of the present application which is described solely by the claims appended below. It should be understood that modifications of the preferred embodiments may be made as would occur to one of skilled in the art. Citada por Patente citante Fecha de presentaci�n Fecha de publicaci�n Solicitante T�tuloUS2011009018223 Dic 201021 Abr 2011Xu JianpingDigital signature collection and authenticationGirarImagen originalP�gina principal de Google - Sitemap - Descargas masivas de USPTO - Pol�tica de privacidad - Condiciones de servicio - Acerca de Google Patentes - Danos tu opini�nDatos proporcionados por IFI CLAIMS Patent Services©2012 Google