WO2021077792A1 - Alloy resistor - Google Patents
Alloy resistor Download PDFInfo
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- WO2021077792A1 WO2021077792A1 PCT/CN2020/099146 CN2020099146W WO2021077792A1 WO 2021077792 A1 WO2021077792 A1 WO 2021077792A1 CN 2020099146 W CN2020099146 W CN 2020099146W WO 2021077792 A1 WO2021077792 A1 WO 2021077792A1
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01C—RESISTORS
- H01C1/00—Details
- H01C1/08—Cooling, heating or ventilating arrangements
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01C—RESISTORS
- H01C1/00—Details
- H01C1/14—Terminals or tapping points or electrodes specially adapted for resistors; Arrangements of terminals or tapping points or electrodes on resistors
- H01C1/1406—Terminals or electrodes formed on resistive elements having positive temperature coefficient
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01C—RESISTORS
- H01C1/00—Details
- H01C1/14—Terminals or tapping points or electrodes specially adapted for resistors; Arrangements of terminals or tapping points or electrodes on resistors
- H01C1/1413—Terminals or electrodes formed on resistive elements having negative temperature coefficient
Definitions
- the present invention relates to the technical field of resistors.
- Resistors as the most common passive components with the most diversified functions in electronic products, are usually required to have more performance and features.
- Current electronic products put forward the following requirements for resistors: high power, high precision, low loss, high reliability and strong adaptability. For resistor manufacturers, simple production processes and short process cycles can greatly improve product competitiveness.
- the resistance element part of the traditional resistor is a two-electrode part.
- Two voltage lines are drawn from the wiring of the PCB board and fed back to the IC terminal, thereby using the voltage difference to calculate the current value, but in the past, the electrode size was enlarged due to heat dissipation requirements. Indirectly compresses the wiring position of the voltage line, causing inconvenience in design and use.
- the resistance value is controlled by the probe for point measurement, which is measured due to the different positions of the probes. The resistance value will have variability.
- there are some 4-electrode designs which divide the electrodes at both ends of the resistor into current electrodes (conductive electrodes) and voltage electrodes (test electrodes).
- the passing current (AC or DC) can be controlled very small, the current electrode will still be polarized, which will affect the accuracy of the test.
- two test electrodes are used for measurement (such as the Wheatstone bridge method), because there is no current through the output terminal. After knowing the distance between the two poles and the cross-sectional area of the object, the resistivity or conductivity of the object can be calculated.
- the problem in this four-electrode design is that the current electrode and the voltage electrode are separated, thereby compressing the space of the current electrode, resulting in poor heat dissipation of the product.
- the present invention provides an alloy resistor with a 4-electrode design, and achieves the effect of high space utilization of the current electrode, so as to improve the heat dissipation of the current electrode.
- the alloy resistor of the present invention can adopt the following technical solutions:
- An alloy resistor comprising a resistance layer, current electrodes connected to both ends of the resistance layer, and voltage electrodes connected to the resistance layer; characterized in that the voltage electrodes are not connected to the current electrodes, and the volume of each current electrode is larger than that of each current electrode. The volume of the voltage electrode.
- the current electrode connected to the resistance layer is larger than the voltage electrode, that is, the space utilization rate of the current electrode is improved to facilitate the heat dissipation of the current electrode.
- Fig. 1 is a schematic side view of the alloy resistor in the first embodiment.
- Fig. 2 is a schematic bottom view of the alloy resistor in the first embodiment.
- Fig. 3 is a schematic side view of the alloy resistor in the second embodiment.
- Fig. 4 is a schematic bottom view of the alloy resistor in the second embodiment.
- Fig. 5 is a schematic bottom view of the alloy resistor in the third embodiment.
- Fig. 6 is a schematic bottom view of the alloy resistor in the fourth embodiment.
- Fig. 7 is a schematic bottom view of the alloy resistor in the fifth embodiment.
- the alloy resistor provided in this embodiment includes a resistance layer 1, a current electrode connected to both ends of the resistance layer 1, a voltage electrode 3 connected to the resistance layer 1; the voltage electrode 3 Not connected to current electrode 2.
- the current electrode 2 is larger than the voltage electrode 3.
- the current electrode 2 and the voltage electrode 3 located at the same end of the resistance layer 1 are both connected to the bottom surface of the resistance layer 1.
- the width of the current electrode 2 is the same as the width 1 of the resistance layer, and the voltage electrode 3 does not exceed the width of the resistance layer.
- the end surface of the current electrode 2 and the end surface of the resistance layer 1 are coplanar.
- the top view of the overall resistor product is a regular square, and the overall structure is compact and regular, which is conducive to the coordination with the PCB board wiring or other components on the PCB board.
- the bottom surface of the current electrode 2 is L-shaped, and the bottom surface of the voltage electrode 3 is square and is located in the L-shaped notch of the current electrode 2.
- the current electrode 2 can be extended in the space not involved by the voltage electrode 3, which is beneficial to increase the volume of the current electrode 2 and stand up for heat dissipation.
- the volume of each current electrode 2 is greater than the volume of each voltage electrode 3.
- the current electrode requires a larger volume to increase the heat dissipation area.
- the voltage electrode mainly measures the voltage signal after the current passes through the resistor body. The voltage electrode does not need to withstand a large current like the current electrode, and the voltage electrode does not need a higher heat dissipation function. Therefore, when the space of the electrode position is limited, the volume of the current electrode 2 at the same end of the resistive layer is larger than the volume of the voltage electrode 3.
- the current electrode 2 and the voltage electrode 3 located at the same end of the resistance layer 1 are both connected to the end surface of the resistance layer 1.
- the width of the current electrode 2 is the same as the width of the resistance layer 1, and similarly, the volume of each current electrode 2 is greater than the volume of each voltage electrode 3.
- the bottom surface of the current electrode 2 is L-shaped, and the bottom surface of the voltage electrode 3 is square and located in the L-shaped notch of the current electrode 2.
- the current electrode 2 is bent on the outside of the current electrode 2 and extends in the width direction to form an L-shape.
- the voltage electrodes 3 provided at both ends of the resistance layer 1 may be located at positions where the two ends of the resistance layer 1 are connected to the same side surface of the resistance layer 1.
- the current electrode 2 and the voltage electrode 3 located at the same end of the resistance layer 1 are both connected to the end surface of the resistance layer 1.
- the width of the current electrode 2 is the same as the width of the resistance layer 1, and similarly, the volume of each current electrode 2 is greater than the volume of each voltage electrode 3.
- the bottom surface of the current electrode 2 is L-shaped, and the bottom surface of the voltage electrode 3 is square and located in the L-shaped notch of the current electrode 2.
- the volume of the current electrode 2 is increased, the length of the overall product is not increased, but is bent on the outside of the current electrode 2 to extend in the width direction to form an L-shape.
- the difference from the second embodiment is that, as shown in FIG.
- one voltage electrode 3 is located at a position where one end of the resistance layer 1 is in contact with one side of the resistance layer 1; the other voltage electrode 3'is located at the position where the other end of the resistance layer 1 and the other side of the resistance layer 1 are connected.
- the current electrode 2 is connected to the bottom surface of the resistance layer 1, or the current electrode 2 is connected to the end surface of the resistance layer 1. on.
- the voltage electrode 3 is connected to the side surface of the resistance layer 1, and the two voltage electrodes 3 are connected to the same side surface of the resistance layer 1.
- the volume of each current electrode 2 is greater than the volume of each voltage electrode 3.
- the current electrode 2 can be made as large as possible under the requirement of compact structure. Improve the heat dissipation effect.
- This embodiment is roughly the same as the fourth embodiment.
- the difference is that, as shown in FIG. 7, the two voltage electrodes 3 are connected to the two sides of the resistance layer 2, that is, the two voltage electrodes 3 are separated from the resistance layer 1.
- the two voltage electrodes 3 are connected to the two sides of the resistance layer 2, that is, the two voltage electrodes 3 are separated from the resistance layer 1.
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Abstract
An alloy resistor. The alloy resistor comprises a resistive layer (1), current electrodes (2) connected to two ends of the resistive layer (1), and voltage electrodes (3) connected to the resistive layer (1), wherein the voltage electrodes (3) are not connected to the current electrodes (2). In addition, the current electrodes (2) connected to the resistive layer (1) are larger than the voltage electrodes (3) connected to the resistive layer, that is, the space utilization rate of the current electrodes (2) is improved to facilitate heat dissipation of the current electrodes (2).
Description
本发明涉及电阻器的技术领域。The present invention relates to the technical field of resistors.
随着电子行业的快速发展,电子产品趋于高可靠性和多功能化,且同时具备运行稳定、损耗低和能适应不同工作环境等特点,这也对电子产品相关的元器件性能提出更多要求。With the rapid development of the electronics industry, electronic products tend to be highly reliable and multifunctional, and have the characteristics of stable operation, low loss and adaptability to different working environments. This also proposes more for the performance of electronic products related components. Claim.
电阻器作为电子产品中最常见、功能最多元化的被动元器件,通常被要求更多的性能和特点。目前的电子产品对于电阻器提出如下要求:大功率、高精度、低损耗、高可靠性和适应能力强等。对于电阻器制造企业来讲,生产工艺简单,制程周期短,都可极大提高产品竞争力。Resistors, as the most common passive components with the most diversified functions in electronic products, are usually required to have more performance and features. Current electronic products put forward the following requirements for resistors: high power, high precision, low loss, high reliability and strong adaptability. For resistor manufacturers, simple production processes and short process cycles can greatly improve product competitiveness.
传统电阻器的电阻元件部分是2电极部分,在PCB板的布线中拉出2条电压线反馈给IC端,藉此利用压差推算出电流值,但以往由于散热的要求将电极尺寸放大,间接压缩了电压线的走线位置,造成设计及使用上的不方便,另外在生产过程中由于在阻值的制程控制都是通过探针做点量测,因探针之位置不同所量测出来的阻值会有变异性,另外有一些4电极的设计,将电阻器两端的电极分为电流电极(导电电极)以及电压电极(测试电极)。虽然通过的电流(交流或直流)可以控制很小,电流电极仍将发生极化,影响测试精度。为此利用两测试电极测量(如惠斯登电桥法),因其输出端无电流通过。知道两极间距离及物体截面积后,即能算出该物体的电阻率或电导率口。但是该种4电极设计中存在的问题是,将电流电极及电压电极分开,进而压缩了电流电极的空间,导致产品散热性变差。The resistance element part of the traditional resistor is a two-electrode part. Two voltage lines are drawn from the wiring of the PCB board and fed back to the IC terminal, thereby using the voltage difference to calculate the current value, but in the past, the electrode size was enlarged due to heat dissipation requirements. Indirectly compresses the wiring position of the voltage line, causing inconvenience in design and use. In addition, in the production process, the resistance value is controlled by the probe for point measurement, which is measured due to the different positions of the probes. The resistance value will have variability. In addition, there are some 4-electrode designs, which divide the electrodes at both ends of the resistor into current electrodes (conductive electrodes) and voltage electrodes (test electrodes). Although the passing current (AC or DC) can be controlled very small, the current electrode will still be polarized, which will affect the accuracy of the test. For this purpose, two test electrodes are used for measurement (such as the Wheatstone bridge method), because there is no current through the output terminal. After knowing the distance between the two poles and the cross-sectional area of the object, the resistivity or conductivity of the object can be calculated. However, the problem in this four-electrode design is that the current electrode and the voltage electrode are separated, thereby compressing the space of the current electrode, resulting in poor heat dissipation of the product.
故,需要一种新的技术方案以解决上述问题。Therefore, a new technical solution is needed to solve the above-mentioned problems.
发明内容Summary of the invention
发明目的:本发明提供一种采用4电极设计的合金电阻器,并实现电流电极空间利用率高的效果,以提高电流电极散热性。Objective of the invention: The present invention provides an alloy resistor with a 4-electrode design, and achieves the effect of high space utilization of the current electrode, so as to improve the heat dissipation of the current electrode.
技术方案:为达到上述目的,本发明合金电阻器可采用如下技术方案:Technical solution: In order to achieve the above-mentioned purpose, the alloy resistor of the present invention can adopt the following technical solutions:
一种合金电阻器,包括电阻层、连接于电阻层两端的电流电极、与电阻层连接的电压电极;其特征在于,所述电压电极不与电流电极相连,每个电流电极的体积大于每个电压电极的体积。An alloy resistor, comprising a resistance layer, current electrodes connected to both ends of the resistance layer, and voltage electrodes connected to the resistance layer; characterized in that the voltage electrodes are not connected to the current electrodes, and the volume of each current electrode is larger than that of each current electrode. The volume of the voltage electrode.
有益效果:本发明中,电阻层连接的电流电极大于电压电极,即提高电流电极的空间利用率以有利于电流电极的散热。Beneficial effects: In the present invention, the current electrode connected to the resistance layer is larger than the voltage electrode, that is, the space utilization rate of the current electrode is improved to facilitate the heat dissipation of the current electrode.
图1是实施例一中的合金电阻器的侧视示意图。Fig. 1 is a schematic side view of the alloy resistor in the first embodiment.
图2是实施例一中的合金电阻器的仰视示意图。Fig. 2 is a schematic bottom view of the alloy resistor in the first embodiment.
图3是实施例二中的合金电阻器的侧视示意图。Fig. 3 is a schematic side view of the alloy resistor in the second embodiment.
图4是实施例二中的合金电阻器的仰视示意图。Fig. 4 is a schematic bottom view of the alloy resistor in the second embodiment.
图5是实施例三中的合金电阻器的仰视示意图。Fig. 5 is a schematic bottom view of the alloy resistor in the third embodiment.
图6是实施例四中的合金电阻器的仰视示意图。Fig. 6 is a schematic bottom view of the alloy resistor in the fourth embodiment.
图7是实施例五中的合金电阻器的仰视示意图。Fig. 7 is a schematic bottom view of the alloy resistor in the fifth embodiment.
实施例一Example one
请结合图1及图2所示,本实施例提供的合金电阻器,包括电阻层1、连接于电阻层1两端的电流电极2、与电阻层1连接的电压电极3;所述电压电极3不与电流电极2相连。电流电极2大于电压电极3。其中,所述位于电阻层1同一端的电流电极2和电压电极3均连接于电阻层1的底面上。且电流电极2的宽度与电阻层宽度1相同,而电压电极3也不超过电阻层的宽度范围,电流电极2的端面与电阻层1的端面上下共面。这样整体的电阻器产品的俯视为规整的方形,整体结构紧凑且规整,有利于与PCB板走线或者PCB板上其他元件的配合。其中,为了在电阻层1的底面合理的提高空间利用率,电流电极2的底面为L形,电压电极3的底面为方形且位于电流电极2的L形缺口中。这样电流电极2在电压电极3不涉及的空间均能够延伸,有利于提高电流电极2的体积而立于散热。在本发明中,每个电流电极2的体积大于每个电压电极3的体积。电流电极需要较大的体积以增加散热面积。而电压电极主要是量测电流通过电阻本体后的电压信号,电压电极的不需要如电流电极一样需要承受大电流,且电压电极不需要较高的散热功能。故在电极位置的空间有限的情况下,位于电阻层同一端电流电极2的体积大于电压电极3的体积。Please refer to Figure 1 and Figure 2, the alloy resistor provided in this embodiment includes a resistance layer 1, a current electrode connected to both ends of the resistance layer 1, a voltage electrode 3 connected to the resistance layer 1; the voltage electrode 3 Not connected to current electrode 2. The current electrode 2 is larger than the voltage electrode 3. Wherein, the current electrode 2 and the voltage electrode 3 located at the same end of the resistance layer 1 are both connected to the bottom surface of the resistance layer 1. Moreover, the width of the current electrode 2 is the same as the width 1 of the resistance layer, and the voltage electrode 3 does not exceed the width of the resistance layer. The end surface of the current electrode 2 and the end surface of the resistance layer 1 are coplanar. In this way, the top view of the overall resistor product is a regular square, and the overall structure is compact and regular, which is conducive to the coordination with the PCB board wiring or other components on the PCB board. Among them, in order to reasonably improve the space utilization rate on the bottom surface of the resistance layer 1, the bottom surface of the current electrode 2 is L-shaped, and the bottom surface of the voltage electrode 3 is square and is located in the L-shaped notch of the current electrode 2. In this way, the current electrode 2 can be extended in the space not involved by the voltage electrode 3, which is beneficial to increase the volume of the current electrode 2 and stand up for heat dissipation. In the present invention, the volume of each current electrode 2 is greater than the volume of each voltage electrode 3. The current electrode requires a larger volume to increase the heat dissipation area. The voltage electrode mainly measures the voltage signal after the current passes through the resistor body. The voltage electrode does not need to withstand a large current like the current electrode, and the voltage electrode does not need a higher heat dissipation function. Therefore, when the space of the electrode position is limited, the volume of the current electrode 2 at the same end of the resistive layer is larger than the volume of the voltage electrode 3.
实施例二Example two
如图3所示,在本实施例中,位于电阻层1同一端的电流电极2和电压电极3均连接于电阻层1的端面上。且电流电极2的宽度与电阻层1宽度相同,而同样的,每个电流电极2的体积大于每个电压电极3的体积。为了提高电流电极2的体积,电流电极2的底面为L形,电压电极3的底面为方形且位于电流电极2的L形缺口中。电流电极2虽然体积增大但是没有增加整体产品的长度,而是 在电流电极2的外侧弯折向宽度方向延伸而形成L形。As shown in FIG. 3, in this embodiment, the current electrode 2 and the voltage electrode 3 located at the same end of the resistance layer 1 are both connected to the end surface of the resistance layer 1. And the width of the current electrode 2 is the same as the width of the resistance layer 1, and similarly, the volume of each current electrode 2 is greater than the volume of each voltage electrode 3. In order to increase the volume of the current electrode 2, the bottom surface of the current electrode 2 is L-shaped, and the bottom surface of the voltage electrode 3 is square and located in the L-shaped notch of the current electrode 2. Although the volume of the current electrode 2 is increased, the length of the overall product is not increased. Instead, the current electrode 2 is bent on the outside of the current electrode 2 and extends in the width direction to form an L-shape.
在本实施例中,如图4所示,可将设置电阻层1两端的电压电极3位于电阻层1两端与电阻层1同一侧侧面相接的位置。In this embodiment, as shown in FIG. 4, the voltage electrodes 3 provided at both ends of the resistance layer 1 may be located at positions where the two ends of the resistance layer 1 are connected to the same side surface of the resistance layer 1.
实施例三Example three
在本实施例中,位于电阻层1同一端的电流电极2和电压电极3均连接于电阻层1的端面上。且电流电极2的宽度与电阻层1宽度相同,而同样的,每个电流电极2的体积大于每个电压电极3的体积。为了提高电流电极2的体积,电流电极2的底面为L形,电压电极3的底面为方形且位于电流电极2的L形缺口中。则电流电极2虽然体积增大但是没有增加整体产品的长度,而是在电流电极2的外侧弯折向宽度方向延伸而形成L形。与实施例二不同的是,如图5所示,在电阻层1两端的电压电极3中,一个电压电极3位于电阻层1一端与电阻层1一侧侧面相接的位置;另一个电压电极3’位于电阻层1另一端与电阻层1另一侧侧面相接的位置。以应对不同的PCB走线要求。In this embodiment, the current electrode 2 and the voltage electrode 3 located at the same end of the resistance layer 1 are both connected to the end surface of the resistance layer 1. And the width of the current electrode 2 is the same as the width of the resistance layer 1, and similarly, the volume of each current electrode 2 is greater than the volume of each voltage electrode 3. In order to increase the volume of the current electrode 2, the bottom surface of the current electrode 2 is L-shaped, and the bottom surface of the voltage electrode 3 is square and located in the L-shaped notch of the current electrode 2. Although the volume of the current electrode 2 is increased, the length of the overall product is not increased, but is bent on the outside of the current electrode 2 to extend in the width direction to form an L-shape. The difference from the second embodiment is that, as shown in FIG. 5, among the voltage electrodes 3 at both ends of the resistance layer 1, one voltage electrode 3 is located at a position where one end of the resistance layer 1 is in contact with one side of the resistance layer 1; the other voltage electrode 3'is located at the position where the other end of the resistance layer 1 and the other side of the resistance layer 1 are connected. To deal with different PCB routing requirements.
实施例四Example four
如图6所示,在本实施例中,位于电阻层1同一端的电流电极2和电压电极3中,电流电极2连接于电阻层1的底面上,或电流电极2连接于电阻层1的端面上。而电压电极3连接于电阻层1的侧面上,且两个电压电极3连接于电阻层1的同一个侧面上。每个电流电极2的体积大于每个电压电极3的体积。在该实施方式中,电压电极3由于连接与电阻层1的侧面,则不影响电流电极2在电阻层1端部连接的空间,能够使电流电极2在结构紧凑的要求下尽量体积做大以提高散热效果。As shown in FIG. 6, in this embodiment, among the current electrode 2 and the voltage electrode 3 located at the same end of the resistance layer 1, the current electrode 2 is connected to the bottom surface of the resistance layer 1, or the current electrode 2 is connected to the end surface of the resistance layer 1. on. The voltage electrode 3 is connected to the side surface of the resistance layer 1, and the two voltage electrodes 3 are connected to the same side surface of the resistance layer 1. The volume of each current electrode 2 is greater than the volume of each voltage electrode 3. In this embodiment, because the voltage electrode 3 is connected to the side surface of the resistance layer 1, it does not affect the space where the current electrode 2 is connected at the end of the resistance layer 1. The current electrode 2 can be made as large as possible under the requirement of compact structure. Improve the heat dissipation effect.
实施例五Example five
本实施例与实施例四大致相同,不同之处在于,如图7所示,两个电压电极3分别连接于电阻层2的两个侧面上,即两个电压电极3被隔在电阻层1的两侧,以应对不同的PCB走线要求。This embodiment is roughly the same as the fourth embodiment. The difference is that, as shown in FIG. 7, the two voltage electrodes 3 are connected to the two sides of the resistance layer 2, that is, the two voltage electrodes 3 are separated from the resistance layer 1. To meet different PCB routing requirements.
本发明具体实现该技术方案的方法和途径很多,以上所述仅是本发明的优选实施方式。应当指出,对于本技术领域的普通技术人员来说,在不脱离本发明原理的前提下,还可以做出若干改进和润饰,这些改进和润饰也应视为本发明的保护范围。本实施例中未明确的各组成部分均可用现有技术加以实现。The present invention has many methods and ways to specifically realize the technical solution, and the above are only the preferred embodiments of the present invention. It should be pointed out that for those of ordinary skill in the art, without departing from the principle of the present invention, several improvements and modifications can be made, and these improvements and modifications should also be regarded as the protection scope of the present invention. All the components that are not clear in this embodiment can be implemented using existing technology.
Claims (10)
- 一种合金电阻器,包括电阻层、连接于电阻层两端的电流电极、与电阻层连接的电压电极;其特征在于,所述电压电极不与电流电极相连,每个电流电极的体积大于每个电压电极的体积。An alloy resistor, comprising a resistance layer, current electrodes connected to both ends of the resistance layer, and voltage electrodes connected to the resistance layer; characterized in that the voltage electrodes are not connected to the current electrodes, and the volume of each current electrode is larger than that of each current electrode. The volume of the voltage electrode.
- 根据权利要求1所述的合金电阻器,其特征在于:所述位于电阻层同一端的电流电极和电压电极均连接于电阻层的底面上,且电流电极的宽度与电阻层宽度相同,电流电极的端面与电阻层的端面上下共面,电流电极的底面为L形,电压电极的底面为方形且位于电流电极的L形缺口中。The alloy resistor according to claim 1, wherein the current electrode and the voltage electrode at the same end of the resistance layer are both connected to the bottom surface of the resistance layer, and the width of the current electrode is the same as the width of the resistance layer, and the width of the current electrode is the same as that of the resistance layer. The end surface is coplanar with the end surface of the resistance layer, the bottom surface of the current electrode is L-shaped, and the bottom surface of the voltage electrode is square and is located in the L-shaped notch of the current electrode.
- 根据权利要求1所述的合金电阻器,其特征在于:所述位于电阻层同一端的电流电极和电压电极均连接于电阻层的端面上,且电流电极的宽度与电阻层宽度相同,电流电极的底面为L形,电压电极的底面为方形且位于电流电极的L形缺口中。The alloy resistor according to claim 1, wherein the current electrode and voltage electrode at the same end of the resistance layer are both connected to the end face of the resistance layer, and the width of the current electrode is the same as the width of the resistance layer, and the width of the current electrode is the same as that of the resistance layer. The bottom surface is L-shaped, and the bottom surface of the voltage electrode is square and is located in the L-shaped notch of the current electrode.
- 根据权利要求1所述的合金电阻器,其特征在于:所述位于电阻层同一端的电流电极和电压电极中,电流电极连接于电阻层的底面或端面上,而电压电极连接于电阻层的侧面上,且两个电压电极连接于电阻层的同一个侧面上。The alloy resistor according to claim 1, wherein among the current electrode and the voltage electrode at the same end of the resistance layer, the current electrode is connected to the bottom surface or end surface of the resistance layer, and the voltage electrode is connected to the side surface of the resistance layer And the two voltage electrodes are connected to the same side surface of the resistance layer.
- 根据权利要求1所述的合金电阻器,其特征在于:所述位于电阻层同一端的电流电极和电压电极中,电流电极连接于电阻层的底面或端面上,而电压电极连接于电阻层的侧面上,且两个电压电极分别连接于电阻层的两个侧面上。The alloy resistor according to claim 1, wherein among the current electrode and the voltage electrode at the same end of the resistance layer, the current electrode is connected to the bottom surface or end surface of the resistance layer, and the voltage electrode is connected to the side surface of the resistance layer And the two voltage electrodes are respectively connected to the two sides of the resistance layer.
- 根据权利要求3所述的合金电阻器,其特征在于:电阻层两端的电压电极位于电阻层两端与电阻层同一侧侧面相接的位置。3. The alloy resistor according to claim 3, wherein the voltage electrodes at both ends of the resistance layer are located at positions where both ends of the resistance layer are connected to the same side surface of the resistance layer.
- 根据权利要求3所述的合金电阻器,其特征在于:电阻层两端的电压电极中,一个电压电极位于电阻层一端与电阻层一侧侧面相接的位置;另一个电压电极位于电阻层另一端与电阻层另一侧侧面相接的位置。The alloy resistor according to claim 3, wherein among the voltage electrodes at both ends of the resistance layer, one voltage electrode is located at a position where one end of the resistance layer is in contact with one side of the resistance layer; the other voltage electrode is located at the other end of the resistance layer The position where it meets the other side of the resistive layer.
- 根据权利要求7所述的合金电阻器,其特征在于:电流电极的外侧弯折向宽度方向延伸而形成L形。The alloy resistor according to claim 7, wherein the outer side of the current electrode is bent and extends in the width direction to form an L-shape.
- 根据权利要求1至8中任一项所述的合金电阻器,其特征在于:电流电极的宽度与电阻层宽度相同,而电压电极也不超过电阻层的宽度范围。The alloy resistor according to any one of claims 1 to 8, wherein the width of the current electrode is the same as the width of the resistance layer, and the voltage electrode does not exceed the width of the resistance layer.
- 根据权利要求9所述的合金电阻器,其特征在于:电流电极的端面与电阻层的端面上下共面。9. The alloy resistor of claim 9, wherein the end face of the current electrode and the end face of the resistance layer are coplanar up and down.
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CN110676006A (en) * | 2019-10-24 | 2020-01-10 | 南京萨特科技发展有限公司 | Alloy resistor |
CN210778077U (en) * | 2019-10-24 | 2020-06-16 | 南京萨特科技发展有限公司 | Alloy resistor |
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