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USRE28597E - Resistor - Google Patents

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USRE28597E
USRE28597E US55109175A USRE28597E US RE28597 E USRE28597 E US RE28597E US 55109175 A US55109175 A US 55109175A US RE28597 E USRE28597 E US RE28597E
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metal foil
base
linear expansion
metal
coefficient
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Priority claimed from US00400345A external-priority patent/US3824521A/en
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01CRESISTORS
    • H01C7/00Non-adjustable resistors formed as one or more layers or coatings; Non-adjustable resistors made from powdered conducting material or powdered semi-conducting material with or without insulating material
    • H01C7/06Non-adjustable resistors formed as one or more layers or coatings; Non-adjustable resistors made from powdered conducting material or powdered semi-conducting material with or without insulating material including means to minimise changes in resistance with changes in temperature
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01CRESISTORS
    • H01C7/00Non-adjustable resistors formed as one or more layers or coatings; Non-adjustable resistors made from powdered conducting material or powdered semi-conducting material with or without insulating material
    • H01C7/22Elongated resistive element being bent or curved, e.g. sinusoidal, helical

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  • ABSTRACT An improved thin-film resistor low in the resistance temperature coefficient is provided.
  • a metal film or foil is bonded with a thermosetting resin onto an insulating base plate having a lower linear expansion coefficient than the metal and is etching-processed so as to be of a desired resistance pattern.
  • the difference in the linear expansion coefficient between the metal and the insulating base is selected to be 26 to 66 X l0 /C.
  • the metal and base are covered with a resin so as to be a molded assembly, together with lead wires connected to both ends of the metal.
  • This invention relates to resistors and, more particularly, to a resistor which is low in the resistance temperature coefficient.
  • Resistors to be used generally for electronic computors, communication instruments, measuring instruments and the like are required to meet such various requirements that the resistance temperature coefficient (which shall bemerely called temperature coefficient hereinafter) should be low, that the allowance of the resistance value should be low, that the size should be small, and so on. 1
  • the resistance temperature coefficient which shall bemerely called temperature coefficient hereinafter
  • the one which can meet the above mentioned requirements will be thin film resistors, or wire-wound resistors in which alloys comparatively low in the temperature coefficient are used.
  • the thin film resistors are made by a vacuum evaporation or cathode sputtering process and, therefore, they have a defect that they are short of a temperature stability as a property peculiar to thin films, that is, as different from bulky metals.
  • the temperature coefficient is 1- several to 1 several 100 p.p.m./C and it is very difficult to make the value of the temperature coefficient smaller.
  • a foil is bonded to a base with an adhesive resin, which resin causes the balance of the force to be broken and thereby there occurs a distortion of the base, and in order to avoid such phenomena Zandman et al. suggest to apply also on the other surface of the base with the same kind of resin to be of the same thickness, whereby such force that tends to bend the base due to the adhesive resin applied thereto will be balanced. Therefore, there are remarkable limitations to the material and dimensions forming the resin layer and the producing conditions are very difficult.
  • the present invention has succeeded in solving the above problems by bonding a metal foil on an insulating base having a lower linear expansion coefficient than the metal so that the resistance temperature coefficient will be reduced by the strain produced in the metal foil by the difference between the respective linear expansion coefficients of both.
  • a main object ofthe present invention is, therefore, to provide a resistor which is very low in the resistance temperature coefficient.
  • Another objectof the present invention is to provide a resistor low in the residual inductance by bonding a metal foil to an insulating base so that the structure will be substantially two-dimensional.
  • the present invention is to provide a resistor stable in the resistance by utilizing the properties of a bulky metal.
  • FIG. 1 shows a heat-treatment curve in the resistor according to the present invention
  • FIG. 2 shows an example of dimensions of the insulating base employed inthe present invention
  • FIG. 3 shows a resistance pattern provided on the base
  • FIGS. 4 and 5 are diagrams showing resistance variation rate due to temperature of the resistors according to the present invention.
  • FIG. 6 shows relations between the temperature coefficient and the difference between the respective linear expansion coefficients of the metal foil (3,) and of the insulating base (B).
  • Ni Cr alloy is rolled to be of a thickness of about 1 to 1014. by a known process.
  • additives thereto Cu, Al, Si and Mn are used to adjust the temperature coefficient and linear expansion coefficient of the alloy. The amounts of the addition of these additives by weight percent are:
  • Such insulating base having a linear expansion coefficient in the range of 40 X 10"/C to 125 X lO"/C which is lower than that of the Ni Cr metal foil as, for example, of borosilicate glass, sintered alumina, soda glass or the like is used.
  • the relation between the thickness of the base and the thickness of the metal foil is selected to be of such a ratio that the thickness of the base the thickness of the metal foil to 1000.
  • the metal foil is then adhered to a surface of such an insulating base as above.
  • An adhesive is thinly applied onto said base.
  • the thickness of the adhesive should be preferably about 10p, and it is also preferable to use an adhesive made of a thermosetting resin.
  • the difference in the linear expansion coefficient B between the base and metal foil is to be effectively utilized.
  • the difference in the coefficient B between the base and metal foil is in the range of 26 to 66 X lO /C. If the difference in the coefficient B is made to be larger than 66 X 10"'/C, only resistancetemperature coefficient as low as in the conventional technique will be obtained. Even if it is made smaller than 26 X 10 /C, only a large value of the resistancetemperature coefficient will be obtained.
  • the metal foil bonded to the base as above is then etching-processed depending on desired resistance pattern of each kind, then the insulating base including the foil of desired insulating pattern is individually cut, lead wires (for example, tin-plated copper wires of a diameter of 0.16 mm.) are welded to it to form terminals. Then the product is adjusted to be of a desired resistance value by trimming. After the adjustment, the thus obtained resistance element is molded with a phenol resin or epoxy resin so as to be enclosed in the molded resin.
  • a metal foil of a thickness of 3p. was made of an Ni Cr alloy of Ni/Cr of 85/15 and additives of 4 percent by weight Cu, 2 percent by weight Al, 1 percent by weight Si and 1 percent by weight Mn, and was heattreated as shown in FIG. 1.
  • a base was of sintered alumina of 48 mm. long, 48 mm. wide and 0.6 mm. thick (see FIG. 2). This base was thinly painted with a bisphenol type denatured epoxy resin and the above mentioned metal foil was bonded to it. It was etched in squares of 6 mm. X 6 mm. as shown in FIG. 3 to form a resistance pattern.
  • 1 is a.
  • the lead wire should be preferably a tinplated copper wire of a diameter of 0.16 mm.
  • the resistance-temperature characteristics in this case were as shown in FIG. 4, in which the abscissa represents the temperature and the ordinate represents the resistance variation.
  • FIG. 5 shows examples of the resistance temperature characteristics of the resistor according to the present invention, showing that the characteristics vary with the difference B of the linear expansion coefficient of the base (of sintered alumina, soda glass or borosilicate glass) at a ratio of Ni/Cr of 35/15.
  • B B the linear expansion coefficient of the base
  • the relations between the difference between them (B B and the temperature coefficient will be as shown in FIG. 6, in which the batched part shows the range which can be used in the present invention. It will be understood hereby that the present invention has excellent characteristics.
  • a resistor comprising an insulating base, a metal foil bonded onto said insulating base with an adhesive, the difference between the linear expansion coefficient of said metal foil and that of said insulating base being 26 to 66 X lO /C, said metal foil being formed in a resistance pattern of a desired length by etching, lead wires connected to the respective ends of said metal foil and a mold covering an assembly of said base, metal foil and lead wires.
  • a resistor according to claim 1 wherein said metal foil is of an Ni Cr alloy of a weight ratio of Ni/Cr of 3.
  • Resistance temperature coefficient (in p.p.m./C] obtained by the ratio of Nl/Cr and the material of the base Weight ratio of Nl/Cr 77/23 80/20 /15

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  • Engineering & Computer Science (AREA)
  • Microelectronics & Electronic Packaging (AREA)
  • Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Non-Adjustable Resistors (AREA)

Abstract

An improved thin-film resistor low in the resistance temperature coefficient is provided. A metal film or foil is bonded with a thermosetting resin onto an insulating base plate having a lower linear expansion coefficient than the metal and is etchingprocessed so as to be of a desired resistance pattern. The difference in the linear expansion coefficient between the metal and the insulating base is selected to be 26 to 66 X 7/*C. The metal and base are covered with a resin so as to be a molded assembly, together with lead wires connected to both ends of the metal.

Description

United States Patent [191 Horii et al.
[111 E Re. 28,597
[ Reissued Oct. 28, 1975 RESISTOR [75] Inventors: Kazuo Horii; Kazuo Ohya; Matuo Zama; Hiroyuki Takashina, all of Tokyo, Japan [73] Assignee: TDK Electronics Co., Ltd., Tokyo,
Japan [22] Filed: Feb. 20, 1975 [21] Appl. No.: 551,091
Related U.S. Patent Documents Reissue of:
[64] Patent No.: 3,824,521
Issued: July 16, 1974 Appl. No.: 400,345
Filed: Sept. 24, 1973 [30] Foreign Application Priority Data Sept. 27, 1972 Japan 47-96904 [52] U.S. Cl. 338/275; 338/254; 338/293 [51] Int. Cl. HOlC 1/034 [58] Field of Search 338/254, 275, 262, 293,
[56] References Cited UNITED STATES PATENTS 1,842,433 l/l932 Terwilligor 338/262 2,692,321 10/1954 Hicks 338/254 3,405,381 10/1968 Zandoran 338/254 Primary ExaminerE. A. Goldberg Attorney, Agent, or Firm Wolfe, Hubbard, Leydig, Voit & Osann, Ltd.
[57] ABSTRACT An improved thin-film resistor low in the resistance temperature coefficient is provided. A metal film or foil is bonded with a thermosetting resin onto an insulating base plate having a lower linear expansion coefficient than the metal and is etching-processed so as to be of a desired resistance pattern. The difference in the linear expansion coefficient between the metal and the insulating base is selected to be 26 to 66 X l0 /C. The metal and base are covered with a resin so as to be a molded assembly, together with lead wires connected to both ends of the metal.
6 Claims, 6 Drawing Figures Reissued Oct. 28, 1975 Sheet 1 of3 Re. 28,597
30/ Wclcl 83L RESISTOR Matter enclosed in heavy brackets I: appears in the original patent but forms no part of this reissue specification; matter printed in italics indicates the additions made by reissue.
This invention relates to resistors and, more particularly, to a resistor which is low in the resistance temperature coefficient.
Resistors to be used generally for electronic computors, communication instruments, measuring instruments and the like are required to meet such various requirements that the resistance temperature coefficient (which shall bemerely called temperature coefficient hereinafter) should be low, that the allowance of the resistance value should be low, that the size should be small, and so on. 1
In conventional resistors, the one which can meet the above mentioned requirements will be thin film resistors, or wire-wound resistors in which alloys comparatively low in the temperature coefficient are used. However, the thin film resistors are made by a vacuum evaporation or cathode sputtering process and, therefore, they have a defect that they are short of a temperature stability as a property peculiar to thin films, that is, as different from bulky metals.
Generally, in the thin film resistors, the temperature coefficient is 1- several to 1 several 100 p.p.m./C and it is very difficult to make the value of the temperature coefficient smaller.
on the other hand in the case of a wire-wound resistor, as the structure of the resistor is three-dimensional, the residual inductance becomes so high that it is difficult to use the resistor in a high frequency range. Further, it is almost impossible to stably manufacture resistors having the temperature coefficient less than fl to 5 p.p.m./C.
There have been already suggested certain measures to solve such defects in the conventional resistors of the kind referred to, for example, in Zandman et al. US. Pat. Nos. 3,405,381 and 3,517,436.
In the techniques suggested in such patents, a foil is bonded to a base with an adhesive resin, which resin causes the balance of the force to be broken and thereby there occurs a distortion of the base, and in order to avoid such phenomena Zandman et al. suggest to apply also on the other surface of the base with the same kind of resin to be of the same thickness, whereby such force that tends to bend the base due to the adhesive resin applied thereto will be balanced. Therefore, there are remarkable limitations to the material and dimensions forming the resin layer and the producing conditions are very difficult.
The present invention has succeeded in solving the above problems by bonding a metal foil on an insulating base having a lower linear expansion coefficient than the metal so that the resistance temperature coefficient will be reduced by the strain produced in the metal foil by the difference between the respective linear expansion coefficients of both.
A main object ofthe present invention is, therefore, to provide a resistor which is very low in the resistance temperature coefficient.
Another objectof the present invention is to provide a resistor low in the residual inductance by bonding a metal foil to an insulating base so that the structure will be substantially two-dimensional.
Further, in a resistor obtained bya vacuum evaporation or cathode sputtering process, as a thin metal film is used, properties'peculiar to such thin film are shown and the resistance is unstable in respect of the temperature. As a further object, the present invention is to provide a resistor stable in the resistance by utilizing the properties of a bulky metal.
The present invention shall now be explained in detail with reference to certain preferred embodiments in conjunction with the accompanying drawings, in which:
FIG. 1 shows a heat-treatment curve in the resistor according to the present invention;
FIG. 2 shows an example of dimensions of the insulating base employed inthe present invention;
FIG. 3 shows a resistance pattern provided on the base;
FIGS. 4 and 5 are diagrams showing resistance variation rate due to temperature of the resistors according to the present invention; and
FIG. 6 shows relations between the temperature coefficient and the difference between the respective linear expansion coefficients of the metal foil (3,) and of the insulating base (B The resistor according to the present invention is made as follows.
An Ni Cr alloy is rolled to be of a thickness of about 1 to 1014. by a known process. The Ni Cr alloy is of Ni/Ct=90/l0 to 70/30 at the weight ratio. As additives thereto, Cu, Al, Si and Mn are used to adjust the temperature coefficient and linear expansion coefficient of the alloy. The amounts of the addition of these additives by weight percent are:
Cu 2 to 5% Al 0.5 to 3% Si 0.5 to 2% Mn 0.5 to 4% A desired linear expansion coefficient of about 136 X l0/C is thus obtained. The metal foil of the alloy thus made and rolled as above is then heat-treated in a vacuum or inert gas. For the heat-treatment, it is desirable to keep the foil at about 600C for 3 hours with the rates of the temperature rise and fall as shown in FIG. 1.
Such insulating base having a linear expansion coefficient in the range of 40 X 10"/C to 125 X lO"/C which is lower than that of the Ni Cr metal foil as, for example, of borosilicate glass, sintered alumina, soda glass or the like is used. The relation between the thickness of the base and the thickness of the metal foil is selected to be of such a ratio that the thickness of the base the thickness of the metal foil to 1000.
The metal foil is then adhered to a surface of such an insulating base as above. An adhesive is thinly applied onto said base. At this time, the thickness of the adhesive should be preferably about 10p, and it is also preferable to use an adhesive made of a thermosetting resin.
Further, in the present invention, the difference in the linear expansion coefficient B between the base and metal foil is to be effectively utilized. For this purpose, it is desirable that the difference in the coefficient B between the base and metal foil is in the range of 26 to 66 X lO /C. If the difference in the coefficient B is made to be larger than 66 X 10"'/C, only resistancetemperature coefficient as low as in the conventional technique will be obtained. Even if it is made smaller than 26 X 10 /C, only a large value of the resistancetemperature coefficient will be obtained.
The metal foil bonded to the base as above is then etching-processed depending on desired resistance pattern of each kind, then the insulating base including the foil of desired insulating pattern is individually cut, lead wires (for example, tin-plated copper wires of a diameter of 0.16 mm.) are welded to it to form terminals. Then the product is adjusted to be of a desired resistance value by trimming. After the adjustment, the thus obtained resistance element is molded with a phenol resin or epoxy resin so as to be enclosed in the molded resin.
An experimental example shall be explained in the following:
A metal foil of a thickness of 3p. was made of an Ni Cr alloy of Ni/Cr of 85/15 and additives of 4 percent by weight Cu, 2 percent by weight Al, 1 percent by weight Si and 1 percent by weight Mn, and was heattreated as shown in FIG. 1. A base was of sintered alumina of 48 mm. long, 48 mm. wide and 0.6 mm. thick (see FIG. 2). This base was thinly painted with a bisphenol type denatured epoxy resin and the above mentioned metal foil was bonded to it. It was etched in squares of 6 mm. X 6 mm. as shown in FIG. 3 to form a resistance pattern. In the drawing, 1 is a. base, 2 is an insulation part, 3 is an etched part, 4 and 5 are terminal parts of the resistance body, 6 and 7 are lead wires which are spot-welded to the terminal parts of the resistance body. The lead wire should be preferably a tinplated copper wire of a diameter of 0.16 mm. The resistance-temperature characteristics in this case were as shown in FIG. 4, in which the abscissa represents the temperature and the ordinate represents the resistance variation.
The results when the ratio was varied and the material of the base was varied were as in Table l.
can be made remarkably low in the case where the difference in the linear expansion coefficient between the metal foil and insulating base is of a certain value. FIG. 5 shows examples of the resistance temperature characteristics of the resistor according to the present invention, showing that the characteristics vary with the difference B of the linear expansion coefficient of the base (of sintered alumina, soda glass or borosilicate glass) at a ratio of Ni/Cr of 35/15. When the linear expansion coefficient of the metal foil is B, and the linear expansion coefficient of the base is B the relations between the difference between them (B B and the temperature coefficient will be as shown in FIG. 6, in which the batched part shows the range which can be used in the present invention. It will be understood hereby that the present invention has excellent characteristics.
What is claimed is:
1. A resistor comprising an insulating base, a metal foil bonded onto said insulating base with an adhesive, the difference between the linear expansion coefficient of said metal foil and that of said insulating base being 26 to 66 X lO /C, said metal foil being formed in a resistance pattern of a desired length by etching, lead wires connected to the respective ends of said metal foil and a mold covering an assembly of said base, metal foil and lead wires.
2. A resistor according to claim 1 wherein said metal foil is of an Ni Cr alloy of a weight ratio of Ni/Cr of 3. A resistor according to claim 2 wherein Cu, Al, Si and Mn are added as additives to said Ni Cr alloy.
4. A resistor according to claim 1 wherein the ratio of the thickness of the insulating base to the thickness of the metal foil is 100 to 1,000 l.
5. A resistor according to claim 1 wherein the linear expansion coefficient of said metal foil is substantially 136 X 10"/C and the linear expansion coefficient of said base is 70 X l0"/C.
TABLE 1 Resistance temperature coefficient (in p.p.m./C] obtained by the ratio of Nl/Cr and the material of the base Weight ratio of Nl/Cr 77/23 80/20 /15 Linear Expansion Coefficient (B, of the metal foil Linear Expansion Coefficient Base (/3 of the base l00 lO /C I l8X7O /C 136x l0 /C Boro 40Xl0"/C Resistance B B,= Resistance fl,fi,= I Resistance B,B,= silicate temperature 60Xl0 /C temperature 78Xl0 /C temperature 96 X1O' /C glass coefficient coefficient coefficient (p.p.m./C): (p.p.m./C): (p.p.m./C): -l to +1 7 to +7 -7 to +7 Sintered 70X10"'/C Resistance B fl F Resistance B -B== Resistance fi,B alumina temperature 30Xl0"/C temperature 48Xl0 /C temperature 66XlO /C coefficient coefficient coefficient (p.p.m./C): (p.p.m./C): (p.p.m./C): -2 to +2 1 to +1 2 to +2 Soda 1 10X10"/C Resistance BF-BF Resistance B -B,= Resistance B,B,= glass temperature 10X1O /C temperature 8Xl0"/C temperature 26X10 /C coefficient coefficient coefficient (p.p.m./C): (p.p.m./C): (p.p.m./C): -10 to +10 6 to+6 3 to +3 6. A resistor according to claim 1 wherein said metal 65 foil is of an alloy of Ni/Cr of 85/15 containing 4 percent by weight Cu, 2 percent by weight AI, 1 percent by weight Si and 1 percent by weight Mn.

Claims (6)

1. A resistor comprising an insulating base, a metal foil bonded onto said insulating base with an adhesive, the difference between the linear expansion coefficient of said metal foil and that of said insulating base being 26 to 66 X 10 7/*C, said metal foil being formed in a resistance pattern of a desired length by etching, lead wires connected to the respective ends of said metal foil and a mold covering an assembly of said base, metal foil and lead wires.
2. A resistor according to claim 1 wherein said metal foil is of an Ni - Cr alloy of a weight ratio of Ni/Cr of 90/10 to 70/30.
3. A resistor according to claim 2 wherein Cu, Al, Si and Mn are added as additives to said Ni - Cr alloy.
4. A resistor according to claim 1 wherein the ratio of the thickness of the insulating base to the thickness of the metal foil is 100 to 1,000 : 1.
5. A resistor according to claim 1 wherein the linear expansion coefficient of said metal foil is substantially 136 X 10 7/*C and the linear expansion coefficient of said base is 70 X 10 7/*C.
6. A resistor according to claim 1 wherein said metal foil is of an alloy of Ni/Cr of 85/15 containing 4 percent by weight Cu, 2 percent by weight Al, 1 percent by weight Si and 1 percent by weight Mn.
US55109175 1972-09-27 1975-02-20 Resistor Expired USRE28597E (en)

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JP9690472A JPS4954846A (en) 1972-09-27 1972-09-27
US00400345A US3824521A (en) 1973-09-24 1973-09-24 Resistor
US55109175 USRE28597E (en) 1972-09-27 1975-02-20 Resistor

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Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0009992A1 (en) * 1978-10-10 1980-04-16 Bakelite Uk Limited Articles from resistance foils and their use
US5304977A (en) * 1991-09-12 1994-04-19 Caddock Electronics, Inc. Film-type power resistor combination with anchored exposed substrate/heatsink
US20100074298A1 (en) * 2008-09-04 2010-03-25 Nyffenegger Johannes F Very high speed thin film rtd sandwich
US10418157B2 (en) 2015-10-30 2019-09-17 Vishay Dale Electronics, Llc Surface mount resistors and methods of manufacturing same
US10438729B2 (en) 2017-11-10 2019-10-08 Vishay Dale Electronics, Llc Resistor with upper surface heat dissipation

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US1842433A (en) * 1928-12-28 1932-01-26 Ward Leonard Electric Co Resistance device and insulator
US2692321A (en) * 1950-12-15 1954-10-19 William M Hicks Resistor
US3405381A (en) * 1965-05-04 1968-10-08 Vishay Intertechnology Inc Thin film resistor

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US1842433A (en) * 1928-12-28 1932-01-26 Ward Leonard Electric Co Resistance device and insulator
US2692321A (en) * 1950-12-15 1954-10-19 William M Hicks Resistor
US3405381A (en) * 1965-05-04 1968-10-08 Vishay Intertechnology Inc Thin film resistor

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0009992A1 (en) * 1978-10-10 1980-04-16 Bakelite Uk Limited Articles from resistance foils and their use
US5304977A (en) * 1991-09-12 1994-04-19 Caddock Electronics, Inc. Film-type power resistor combination with anchored exposed substrate/heatsink
US20100074298A1 (en) * 2008-09-04 2010-03-25 Nyffenegger Johannes F Very high speed thin film rtd sandwich
US8118485B2 (en) * 2008-09-04 2012-02-21 AGlobal Tech, LLC Very high speed thin film RTD sandwich
US10418157B2 (en) 2015-10-30 2019-09-17 Vishay Dale Electronics, Llc Surface mount resistors and methods of manufacturing same
US10438729B2 (en) 2017-11-10 2019-10-08 Vishay Dale Electronics, Llc Resistor with upper surface heat dissipation

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