Diagnosis of engine coolant temperature gauge issue with a certain vehicle discussed ECT sensors in a specific context.
The following table of coefficients for four common sensors was derived from published measurements by TSD of a single sensor of each type.
The so-called B equation model is \(T=\frac{1}{\frac1{T_0}+\frac1Bln\frac{R}{R_0}}\).
| Part | R25 | B25/100 |
| AMR3321 | 2246 | 3897 |
| ERR2081 | 2218 | 3879 |
| ETC8946 | 2450 | 3671 |
| AMR1425 | 536 | 4356 |
These are measurements of a single sample, so average values might be a little different. Additionally, the R25 / B25/100 model is only an approximation.
Steinhart-Hart model
This article shows a curve fit of the measurements of the two most common of those sensors to the Steinhart-Hart model of a NTC thermistor. Also shown on the graphs is a plot of calculated temperature using the simpler B equation based on measurements around 20° and 100°.
The Steinhart-Hart model is \(T=\frac{1}{a+b(ln(R))+c(ln(R))^3}\). It is a little more complicated to calculate than the simpler B equation, so less used in simple digital systems.
Above is the AMR3321. The fit is a very good one to the measured data, and as it happens, the B equation is a very good estimator.
Above is the AMR1425. The fit is a quite good one to the measured data, and as it happens, the B equation is a good estimator, but not as good as in the AMR3321.
This is inconsequential with a typical analog gauge which can be scaled to suit the sensor, but it becomes more relevant to a digital application that tries to use a simple equation to relate resistance to temperature.