Resistance and Offset Cancellation in a Remote-Junction Temperature Sensor
US-2015003490-A1 · Jan 1, 2015 · US
US9772231B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-9772231-B2 |
| Application number | US-201414286482-A |
| Country | US |
| Kind code | B2 |
| Filing date | May 23, 2014 |
| Priority date | May 23, 2014 |
| Publication date | Sep 26, 2017 |
| Grant date | Sep 26, 2017 |
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In one example, a method includes determining, by a device, a plurality of voltage values that each correspond to a respective voltage drop across a remote p-n junction while the remote p-n junction is biased at different respective current levels, wherein each of the plurality of voltage values is a function of at least: one of the different respective current levels, a temperature of the remote p-n junction, and a series resistance between the device and the remote p-n junction. In this example, the method also includes, determining, by the device, an intermediate value based on a difference between at least three voltage values of the plurality of voltage values, wherein the intermediate value is not a function of the series resistance, and determining the temperature of the remote p-n junction based on the intermediate value such that the temperature is not a function of the series resistance.
Opening claim text (preview).
The invention claimed is: 1. A method comprising: determining, by a device, a plurality of voltage values that each correspond to a respective voltage drop across a remote p-n junction while the remote p-n junction is biased at different respective current levels, wherein each of the plurality of voltage values is a function of at least: one of the different respective current levels, a temperature of the remote p-n junction, and a series resistance between the device and the remote p-n junction; determining, by the device, an intermediate value based on a difference between at least three voltage values of the plurality of voltage values, wherein the intermediate value is not a function of the series resistance; and determining, by the device, the temperature of the remote p-n junction based on the intermediate value such that the temperature is not a function of the series resistance. 2. The method of claim 1 , wherein the temperature is determined approximately according to the following equation: T = ( V be 1 - V be 2 ) - ( V be 3 - V be 4 ) · K q · ln ( I D 1 · I D 4 I D 2 · I D 3 ) wherein V be1 is a first voltage value of the at least three voltage values, V be2 is a second voltage value of the at least three voltage values, V be3 is a third voltage value of the at least three voltage values, V be4 is a fourth voltage value of the at least three voltage values, is a property of the remote p-n junction, K is the Boltzmann's constant, T is the temperature of the remote p-n junction, q is the elementary charge constant, I D1 is the current level at which the remote p-n junction was biased while the first voltage value was determined, I D2 is the current level at which the remote p-n junction was biased while the second voltage value was determined, I D3 is the current level at which the remote p-n junction was biased while the third voltage value was determined, and I D4 is the current level at which the remote p-n junction was biased while the fourth voltage value was determined. 3. The method of claim 1 , wherein the temperature is determined approximately according to the following equation: T = V be 1 - V be 2 - ( V be 3 - V be 1 ) · K q · ln (
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