Improvements relating to heater systems

Abstract: A heater system provides a portable lightweight tool including the core and at least the primary winding of a transformer having a secondary that may be permanently or selectively coupled to a heater having a bifilar winding to reduce magnetic radiation; wherein the design of the system is such that voltages produced in the portable tool do not materially exceed 100 volts and are normally below 100 volts. The core of the transformer when employed in an arrangement wherein the secondary winding is permanently connected to the heater winding has a leg rotatable out of the closed core configuration whereby another leg of the core having the primary winding wound thereon may be inserted into the secondary winding. Alternatively the secondary winding may be wound on a short length of the core that is insertable into a leg of the transformer core on which the primary winding is wound.

Description: The present invention relates to heater systems, such as are employed in the fusion coupling of plastics materials, and more especially to a portable transformer - link coupling apparatus for mating with a heater embedded in plastics couplings, the apparatus preferably being operable with heaters of many different sizes and construction. Clamshell type structures for effecting fusion of pipes are well known in the art being disclosed in various documents such as WO 8002124 wherein overlapping plastic pipes have a ferromagnetic material located in the overlap region which is excited by a magnetic field carried in a clamshell having a coil therein. U.S. Patent No. 4,914,267 discloses a clamshell heater for fusing solder to effect a solder joint between wires. There are numerous types of clamshell coils or heaters but each is tailored to a specific device, a pipe of a given dimension or other object of given structure and/or dimensions. Thus there must be a clamshell for each such size or shape of structure to be heated or fused, a costly approach and one which becomes unwieldy as the pipes or other structures become large. A further problem is that it is difficult to achieve close fitting clamshell heaters with a low Q so that the prior devices are relatively inefficient, the voltages are high and a series resonant capacitor is required in all instances. The result of all this is that the clamshell is unwieldy, costly and produces high voltages that must be handled with great care. A close fitting solenoid coil can provide lower Q's than the clamshell devices but it requires both mechanical and electrical connections and high voltages since the coupling coefficients are not more than 0.6. The current approaches to fusion coupling do not provide common elements for pipes, saddles, tees or patches so that a special tool is required for each. The invention seeks to achieve a single tool that can accommodate a wide range of heaters both in size, shape and power. Another object of the invention is to achieve a tool structure for effecting fusion coupling of plastics pipes or like uses, that has low electromagnetic radiation. According to one aspect of the present invention, there is provided a heater system comprising a coupling member for producing fusion of members one to the other, an eddy current, temperature self-regulating heater incorporated with said coupling member and having a regulated temperature to heat said member to fusion temperature below a temperature damaging to said coupling member, said heater being comprised of a metallic structure which provides substantial resistance heating from skin effect when operated at high frequency, a transformer having a soft magnetic core and primary and secondary windings disposable on said core, means coupling said secondary winding to said heater structure, said heater structure alone having a Q of between 0.5 and 5, said secondary winding having a reactance such that the ratio of its reactance to the resistance of the heater structure is between 1 and 20, a tool including at least said transformer core and said primary winding, and means for connecting said primary winding to a source of high frequency current. The heater system preferably comprises the heater having bifilar windings. Said primary winding is preferably permanently wound on said core. Preferably, the heater structure has an outer surface of ferromagnetic material, said ferromagnetic material providing a high resistance to passage of high frequency current to produce eddy current heating. In its preferred embodiment, the present invention provides a portable tool which may be linked to heaters of many different sizes, configurations, power requirements and fusion couplings. Important features of such a device are that it can be transformer linked to heaters embedded in couplings, it should preferably operate at voltages below 100 volts and should preferably be able to accommodate heaters of widely different power requirements; for instance, but without limitation, from 500 watts to 1,800 watts. The term "ferromagnetic" as employed herein is used for purposes of simplicity and is intended to cover ferromagnetic, ferrimagnetic and like materials that exhibit a marked decrease in magnetic permeability at their effective Curie temperatures. This latter term relates to the fact that a substantial reduction in heating effect occurs at temperatures below true Curie temperature. Effective Curie temperature may be as little as 1° or as great as 100° below true Curie temperature depending upon the ferromagnetic material employed. To accomplish the objects of the present invention a round cross-section ferromagnetic or ferromagnetic coated wire may be employed. A heater employing such a wire can have an internal Q of between 0.5 and 5.0. If a bifilar winding is employed internal heater Qs of between 0.5 and 1.2 may be achieved. If a helical heater winding is employed the Q may go as high as 10. The transformer secondary in the preferred embodiment of the invention may be permanently connected and embedded in the structure (usually a plastic) with the heater. The secondary winding should be accessible to the core of the transformer and thus the structure may have the appearance of a coffee mug in which the handle includes the secondary winding. The secondary winding of the transformer is chosen such that Q 2 the ratio of its reactance to the resistance of the heater is between 1 and 20. In this way, the objects of the present invention are met. Preferred features of the invention that improve the overall performance of the basic system are the use of a soft magnetic core for the transformer, the use of bifilar windings and the disposition of the primary and secondary windings on the same leg of the core to provide a coupling factor of at least 0.95. The apparatus defined above eliminates the use of external electrical connections and thus the problems incident to achieving proper contact; corrosion, sparking and the like. There may be installations, however, where access to a secondary winding integral with the heater is not physically possible. In such a case the secondary winding may be integral with the primary winding and core and the leads from the secondary winding can be plugged into contacts connected to the heater input leads. Regardless of the disposition of the transformer secondary winding it is strongly preferred, as indicated above, that it be located on the same leg of the core as the primary winding to provide the required coupling coefficient. The heater windings may comprise a plurality of cross coupled parallel wires to reduce resistance and a like return arrangement of wires (bifilar winding) to at least partially cancel the external magnetic fields generated to thereby greatly reduce EMI. Many variations of this basic pattern are possible with the resistance of the heater being lowered as the number of wires in each parallel wire group is increased. The heater thus employed may be of the type disclosed in co-pending U.S. patent application Serial No. 07/657,996 filed by Ross et al on February 20, 1991 for "System and Method for Joining Plastic materials". These heaters are, in the preferred embodiment of the invention, permanently connected to the secondary winding of a transformer and permanently embedded in one of the plastic members to be fused to at least one other such member. The embedded structure is such, however, that the core of the transformer in one embodiment of the invention forming a part of the portable tool and carrying the primary winding may be passed through the turns of the secondary winding to produce the necessary link to couple the embedded members of the system to the external members, thus the term "link coupling". In a second embodiment of the structure where the secondary winding is permanently connected to the heater, a short length of the transformer core is included with the secondary winding in the heater structure, the main body of the core having a gap that snugly receives the short length of core associated with the secondary winding. Alternatively, due to physical constraints, the secondary winding may be a permanent part of the tool and may plug into the heater. The preferred transformer core material is a low loss ferrite to reduce losses such being the result of the very high resistivity of such material. The above structure of the heater and the transformer, the latter preferably having a gap in its magnetic core to prevent saturation of the core, lead to a low Q, low inductance and low resistance system and as such low voltages may be employed to provide power of 1800 watts or higher. It should be noted that a low Q requires that the inductive reactance of the system must be low and the resistance high. Therefore a tradeoff occurs between these two factors. Arrangements for carrying the invention into effect will now be described in more detail by way of example, and with reference to the accompanying drawings, in which: Figure 1 illustrates a basic transformer-load circuit employed for analysis of the heater system of the present invention; Figure 2 is a plot of the Q of the heater system of the invention as a function of the inductance of the secondary winding, inductance of the heater, the coupling factor between the primary and secondary windings and the load resistance; Figure 3 is a plot of the effect of solid wire skin effect quantities on the internal Q of a round wire; Figure 4 is a diagram of a core to be employed with a primary winding wound on one limb thereof; Figure 5 illustrates one form of bifilar heater winding; Figure 6 illustrates a second form of bifilar heater winding; Figure 7 illustrates a birdcage bifilar heater winding; Figures 8a and 8b illustrate still another form of bifilar heater winding; Figure 9 provides three graphs, inductance, resistance and Q of the heater winding as a function of frequency of the supply; Figure 10 illustrates an experimental core and winding arrangement; Figure 11 illustrates the results of the test of the structure of Figure 10; Figures 12a and 12b illustrate a core arrangement that permits insertion of a leg of the core into a secondary winding permanently connected to the heater winding; Figure 13 illustrates an alternative arrangement for coupling a secondary winding of the transformer employed, to the core of the transformer; Figure 14 illustrates a birdcage heater and transformer connection arrangement; and Figures 15a, 15b and 15c illustrate three different heater configurations tested to provide the data for Table 4. Referring to Figure 1 of the accompanying drawings, an analysis is undertaken to demonstrate the approach to achieve a quite low circuit Q. An analysis of the circuit produces the following initial equation: Z = jωL 1 + (ωM) 2 jωL 2 + jωL 3 + R 3 where R 3 is the heater resistance, M is the mutual inductance of the structure, L 1 and L 2 are the inductance of the primary and secondary windings of the transformer, and L 3 is the inductance of the heater. It will be shown how Q can be made quite low and L 1 can be designed to be low enough that the exciting voltage can be held low, below 100 volts. From Equation 1, Equation 2 is developed Q = Q 2 2 + Q 3 2 + 2Q 2 Q 3 + 1 K 2 Q 2 - Q 2 - Q 3 where Q is the Q of the entire circuit, Q 2 = ωL 2 / R 3 and Q 3 = ωL 3 / R 3 and K = M / √L 1 , L 2 . Equation 2 can be reduced to: Q = 1 + 2 Q 2 assuming that both K and Q 3 have values of 1 or very close to 1. The factor K is the coupling factor which can be from 0.95 to virtually 1. For a value of Q 2 = 2, Q 3 = 1.2 and K = 0.95 the Q of the system becomes 2.72. A plot of the value of Q against Q 2 with Q 3 = 1.2, is illustrated in Figure 2 for various values of K. It is seen from Figure 2 that if Q 2 is designed to be between 2 and 10, then Q will be less than 3, an acceptable value. The value of Q 3 , the Q of the heater, is determined in part by the inherent internal Q of a round wire from which the heater is fabricated. This factor is set forth in the graph of Figure 3 in which the lower curve is the factor ωL 1 / R h f . It is noted that the internal Q of the wire is 0.5 at the radius to to depth of penetration ratio of 1 of an eddy current, self regulating round wire. At a ratio of 5, the Q becomes a constant of 1. The Q of the heater is increased by its external Q and in the analysis employed to develop the graphs of Figure 2, a Q 3 = 1.2 was assumed. It is noted from Figure 2, that with a maximum value of Q of approximately 3, the ratio of XL 2 /R 3 , that is, Q 2 can have a value of 1 to 20 which produces this practical maximum. Referring now to the design of the system, low voltage in the portable tool can be achieved since a low Q together with complete freedom in design of the inductive reactance X L1 readily permits attainment of this end. Q 2 is a function among other things, of design of the secondary winding, Q 3 will run between 1 and 3, and the resistance r 3 is made as low a value as possible. There are limitations, however, in the design of this element as will be seen subsequently. As stated above the factors that can be readily controlled are Q 2 and X L1 . The above statement is summarized in Equation 4 as follows: r 1 = K 2 Q 2 Q 2 2 + Q 3 2 + 2Q 2 Q 3 + 1 X L1 from which Equation 1 was derived. As indicated immediately above Q 2 and X L1 are the readily controllable parameters and these are now discussed. V 1RMS = √P h r 1 (1+Q 2 ) where P h is the power generated in the heater. Reference is now made to Figure 4 which illustrates a design of the primary winding and the ferrite core useful in analyzing the design of the system parameters. It can be shown that for the structure illustrated in Figure 4 NA = LI max B max where N is the number of turns of the primary winding, A is the cross-sectional area of the ferrite core, L is the inductance of the primary winding and B max is the maximum flux density in the core where the core is operating over a linear region below saturation. To achieve the maximum current required without producing saturation it is often required to introduce an air gap in the core, such a gap designated in Figure 4 as 1 gap. In the above equation, L is taken to be N 2 µµ 0 A 1 + µ| gap . The factor µ 0 = 4πx10 -7 MKS units. B max and µ are determined by the core chosen. Reference is made to Table 1 which sets forth target values for three heater powers with the system operated at 300 KHz. This table presumes a Q 3 = 1.2, a Q 2 of about 5, L = 1.35 microhenries and K = 0.95. The calculation to produce this table assumed B max = 0.2 Tesla and µ = 3000. The material used is a ferrite supplied by TDK and designated H7C4. The power dissipated per volume at 0.2 Tesla and 300 KHz is 2.5 watts/cm 3 in the core. Power (watts) L (microH) X T (ohms) r (ohms) I rms (amps) V rms (volts) 550 1.35 2.54 0.29 43.5 34.5 900 1.35 2.54 0.29 55.6 44.2 1800 1.35 2.54 0.29 78.6 62.5 It is noted that the rms voltage at maximum power is well below 80 volts, a reference level set by electrofusion technology. Referring to Equation 6, I max may be at least 1.4 times I rms , NA is taken as 742.5 mm 2 and using various combinations of l, l gap , A and NB, Table 2 is generated. 1= 300 mm I max = 135 amps 1 gap = 5 mm yield V max = 339 volts A= 150 sq mm L= 1.33 microH N= 6 turns It can be seen that with the factors chosen as set forth above the factors permitted by the structure I max , V max and L are well above those required to produce the desired heating wattage set forth in Table 1 above. The core tested was not more than 3-1/2 inches on a side with a cross-section of 1/2" x 1/2". The total power dissipated would be 113 watts if operated at the maximum current which it would not be. The maximum values required to produce the desired powers are I max = 78.6A, V max = 62.5V and L = 1.33 microH. The above calculations demonstrate that a relatively small application tool can operate on even large couplings of high wattage. The final design criteria is determined by the heater per se. To minimize external flux radiation bifilar windings may be employed. To provide a low value of resistance each leg of the heater winding is made up of several parallel wires. To prevent the current from concentrating in only one of the wires, cross members are arrayed along the lengths of the parallel wires. These wires also add strength to the structure. Reference is now made to Figure 5 of the accompanying drawings for an illustration of a bifilar winding according to the present invention. The winding comprises a first section 2 comprised of three parallel wires 4, 6 and 8 interconnected by cross-wires all designated by the reference numeral 10. A second section 12 together with section 2 completes the bifilar winding. The section 12 also has three lengths of parallel wires, designated 14, 16 and 18 with cross-wires all designated by the reference numeral 20. The first and second section 10 and 20 are illustrated as cross coupled by three wires designated by numeral 22. The three wire bifilar system provides low resistance, low inductance and low magnetic radiation. A scheme having even lower resistance is illustrated in Figure 6 which employs six wires in each section. The windings 24 or legs 26, 28, etc. of the winding are wound in a spiral fashion and as in Figure 4 each pair of legs of the winding are shorted together at one end. The cross-wires may be replaced by periodically crossing one of the wires in a leg over the others and spot welding it to the others to provide essentially the same operation as the use of cross wires. Referring to Figure 7 two birdcage heaters 30 and 32 of the general type disclosed in the aforesaid Ross et al application, may be connected at one end of each by wires 34 to provide the two sections of the bifilar winding. These two birdcages can encircle the member to be heated providing a very low resistance and a bifilar effect. Basic single wire bifilar winding is illustrated in Figures 8a and 8b and comprises a wire or leg 36 and return wire 38. These figures are illustrated for purposes of analyzing the graphs of Figure 9. The three graphs of Figure 9 compare like performance of the bifilar windings of Figure 5 and Figure 8b as a function of frequency, each heater being five feet long. It is readily apparent from these graphs that the inductance and the resistance of the three wire heater are consistently lower than those for the single wire heater. The Q of the three wire heater is greater than that of the single wire heater but the difference even at 300 KHz is only 1.27 times that of the single wire heater. The resistance and inductance of the single wire heater on the other hand are roughly two to three times that of the three wire heater. The above equations have basically defined a system according to one embodiment of the present invention. Reference is made to Figure 10 of the accompanying drawings. Rectangular soft ferrite blocks 40, 42, 44 and 46 were taped together to form an ungapped core. Each block measured 2-1/8 x 13/16 x 11/32 inch. The primary winding 48 had two turns and secondary winding 50 had three turns. The secondary winding was connected to the three wire heater of Figure 5. Measurements were made at 100 KHz using a Digibridge. Measurements were L 1 = 5.27 microH and L 2 = 11.9 microH. The coupling coefficient separately measured was 0.96 with the windings on the same leg and adjacent one another. Table 3 presents the results of the test with and without a 4 ohm carbon resistor in series with the heater. L (uH) Q R (ohms) Q 2 L 3 (uH) Q 3 R 3 (ohms) heater 2.53 2.82 0.56 1.83 8.10 1.24 4.13 w/4 ohms 3.25 2.32 0.875 0.93 8.09 0.63 8.11 Referring to Figure 11 a plot of experimental data corresponding to that of calculated data in figure 2 shows a very close correlation of the two graphs. Of importance is the fact that the objectives of the invention have been met by even the crude model of Figure 10. There is a tradeoff between system Q and system resistance in determining which parameter has the greatest effect on input voltage. An examination of Equation 5 indicates that system resistance has less effect on input voltage than Q since this latter term is squared. Thus in the design of the heater of the present invention, it is preferable to minimize Q even if this means that system resistance is raised. In an alternative arrangement as illustrated in Figures 12a and 12b of the accompanying drawings, the secondary winding is a part of the permanent installation and the core is hinged to permit the core to be inserted into the secondary winding. In Figure 12b the core comprises a generally U-shaped member 66 having a short leg 68 that passes through secondary coil 70, a base leg 72 and a long leg 74 generally parallel to leg 68. Hinged to the bottom of leg 74 by hinge 75 is a leg 76 generally parallel to leg 72 and in the form of an "L". A gap 78 is formed between the part 80 of leg 76 that is parallel to leg 74 and the end of leg 68. A primary winding is preferably disposed on leg 74 or 72 to produce closer coupling to coil 70. The coil 70 is illustrated as having two turns but it may have as little as one turn or in some unusual cases, three turns. When it is desired to insert the core 66 into the secondary winding 70, the leg 76 is rotated downwardly as illustrated in Figure 12a so that the leg 68 may be readily inserted into the coil 70. Once leg 68 is inserted, leg 76 is rotated back into the position illustrated in Figure 12b. A latching mechanism (not illustrated) is provided for leg 76 and mating of the legs 74 and 76 must be very tight tolerances to achieve all that is available from this structure. Referring now to Figure 13 there is illustrated an alternative arrangement for permitting a secondary winding of the transformer that is permanently connected to the heater to be inserted in the core. Specifically a part 80 of core 82 is permanently associated with secondary winding 84. The core 82 has a gap 85 in the leg 86 carrying primary winding 88. The gap 85 is as wide as the core part 80 so that the part 80 is snugly received between the two sides of the core defining the gap. If a gap is desired in the core, a region 90 of the core part 80 may be paramagnetic thus defining the desired gap. If a gap is not desired, then all of the core part 80 is ferromagnetic or ferrimagnetic. An advantage of the construction of the transformer of Figure 13 as opposed to the transformer of Figure 12 is that in Figure 13 the leg on which the secondary is wound need not be straight. The core of the device of Figure 13 may be circular, triangular or of other geometric shape so long as the section of the core on which the secondary is wound is snugly received in the remainder of the core immediately adjacent the primary winding. It should be noted that the core of Figure 12 could also be curved but such configuration would not be as convenient as straight legged cores. Referring now to Figure 14 of the accompanying drawings, a heater 51 comprised of two birdcages 52 and 54 arranged to form a bifilar arrangement is excited by a secondary winding 56 of transformer 58 having a soft ferrite core 60 of the type illustrated in Figure 10 or 12b. The birdcages are arranged as illustrated in Figure 7 but are formed into cylinders, see Figure 14. In this particular arrangement, the secondary winding 56 forms part of the portable tool and is connected in conventional fashion to terminals 62 and 64 of the heater. Figures 15a, b and c illustrate three different heater configurations as indicated in the drawings and tested for the various parameters set forth in Table 4 below. The tests were conducted at low power at 350 KHz with a two turn primary and one and two turn secondaries. A series resonating capacitor to lower the Q of the circuit was then connected in series in the primary winding circuit. The heaters were then operated in air at high power and all three ran at startup at about 2500 watts out of the outlet giving about 2000 watts at the link system. Equibrium was reached at about 1500 watts at the outlet. If operated in a plastic sleeve the wattage would have been 1800 watts. Heater Type Heater Inductance Heater Resistance Q 3 Q 2 Q r 1 Calc. V rms 1800 watt Version 1 1 turn secondary 0.4 µH 0.3Ω 2.7 11 7.2 0.6Ω 245 V Version 2 1 turn secondary 2.0µH 3.2Ω 1.4 1.0 6.7 1.4Ω 310 V Version 2 2 turn secondary 2.0µH 3.2Ω 1.4 3.0 3.6 1.4Ω 200 V Version 3 1 turn secondary 1.0µH 1.1Ω 1.8 2.9 5.8 1.1Ω 250 V Version 3 2 turn secondary 1.1µH 1.1Ω 1.8 8.4 6.1 0.6Ω 200 V It is noted that the primary input voltage calculated for an 1800 watt heater ran from 200 volts to 310 volts. If a single turn primary were used the turns ratio would be reduced by a factor of 4 and each of the calculated voltages would be halved, providing 100 volts in two of the units with a device that was not optimized in design. Thus the theories underlying the present invention are proven. For example, heater wires with cross sectional shapes other than round may also be used.

Claims: A heater system comprising a coupling member for producing fusion of members one to the other, an eddy current, temperature self-regulating heater (51) incorporated with said coupling member and having a regulated temperature to heat said member to fusion temperature below a temperature damaging to said coupling member, said heater being comprised of a metallic structure which provides substantial resistance heating from skin effect when operated at high frequency, characterised in that the system further comprises a transformer (M) having a soft magnetic core (40,42,44,46;66;80,82,86) and primary (88;48) and secondary (84;56;69/70) windings disposable on said core, means for connecting said primary winding to a source of high frequency current, said transformer core and said primary winding constituting a tool, means (62,64) coupling said secondary winding to said heater structure, said heater structure alone having a Q of between 0.5 and 5, and said secondary winding has a reactance such that the ratio of its reactance to the resistance of the heater structure is between 1 and 20. A heater system according to claim 1 wherein said heater is a bifilar winding (2,12; 30,32; 52,54). A heater system according to claim 2 wherein said bifilar winding comprises at least two pairs (2,12;30,32; 52,54) of a plurality of substantially parallel wires (4,6,8,14,16,18) interconnected at spaced points (10,20) along their paths, said pairs interconnected (22) to provide bifilar windings. A heater system according to claim 3 wherein interconnection of said parallel wires comprises a plurality of individual cross members (10,20), connected to each of the parallel wires. A heater system according to claim 3 wherein interconnection of parallel wires is provided by having one of said parallel wires cross the other of the parallel wires at spaced points along said parallel wires. A heater system according to any preceding claim, wherein said secondary winding is permanently connected to said heater, and said secondary winding when said heater is to be energized is disposed on said core. A heater system according to any of claims 1 to 6, wherein said secondary winding is selectively closely couplable to said primary winding. A heater system according to 7 wherein said secondary winding is permanently wound on a short length (80) of said core separable from the remainder (82) of said core, said short length of core being snugly receivable in a leg (86) of said core on which said primary winding is wound. A heater system according to claim 7, wherein said transformer core has a generally rectangular configuration with one leg (76) hinged to the remainder (74) of the core, said one leg being movable away from an adjacent leg (68) such that said adjacent leg may be inserted into said secondary winding (69/70) and said one leg returned to a position completing the magnetic path through the core. A heater system according to claim 9, wherein said primary winding is disposed on another adjacent leg (74). A heater system according to claim 9, comprising means (78,90) to minimize saturation of said core. A heater system according to claim 11, wherein said means is a gap between the movable and adjacent legs. A heater system according to any preceding claim, wherein the Q of said heater system is defined by the equation Q = Q 2 2 + Q 3 2 + 2Q 2 Q 3 + 1 K 2 Q 2 - Q 2 - Q 3 wherein Q 2 is the Q of the secondary winding, Q 3 is the Q of the heater and K is the coupling factor between primary and secondary windings. A heater system according to claim 1 wherein said primary and secondary windings are on the same leg of the transformer core. A heater system according to any preceding claim, wherein said primary winding is permanently wound on said core. A heater system according to any preceding claim, wherein said primary winding is a single turn winding. A heater system according to claim 15, wherein said core and said primary winding constitute a portable member. A heater system according to any preceding claim, wherein said heater structure has an outer surface of ferromagnetic material, and said ferromagnetic material provides a high resistance to passage of high frequency current to produce eddy current heating.

Inventors: DOLJACK FRANK A, DOLJACK, FRANK A.
Applicants: UPONOR ALDYL CO, UPONOR ALDYL COMPANY
Application year: 1993
Main classification: H05B6
IPC codes: H05B6, B29C65