See the relationship before changing it
Set the input, apply the rule, then read the result with its unit.
The retained audit below checks several chapter fixtures. This model keeps those stated values fixed and changes only thermistor resistance, so the numeric fixture does not switch without explanation.
Derive the baseline in four named moves
- 1
Name the input. The chapter baseline is 10000 ohm.
- 2
Name the relationship. T = 1/(1/298.15 + ln(R/10,000)/3,950) - 273.15
- 3
Substitute with units. R = 10,000 ohm gives 25.0 degrees C
- 4
Read the result. Keep the unit beside the value. Use it only inside the technical boundary on this page.
Predict, then change thermistor resistance
Try Predict the direction of T = 1/(1/298.15 + ln(R/10,000)/3,950) - 273.15. Test another thermistor resistance, then compare beta-model temperature.
Observe An NTC thermistor maps lower resistance to higher temperature. Reset thermistor resistance to 10000 and compare beta-model temperature.
Explain The thermistor's resistance falls as heating releases more charge carriers, so larger resistance corresponds to lower temperature through the logarithmic Beta-model conversion.
Check yourself
What should you do before trusting a moved-control result?
What does this small model leave out?
1. See B as a shape control
An NTC thermistor loses resistance as it warms. The B value controls how sharply the exponential curve bends; it is not a fixed percent-per-degree slope.
2. Convert Celsius first
The Beta equation uses reciprocal absolute temperature. Using Celsius inside 1/T would produce a physically meaningless result.
3. Follow the curve and its slope
The slope magnitude falls as T² grows. Multiplying B by Boltzmann's constant also expresses the chapter's material parameter as an activation energy.
4. Try the temperature
TryWarm the chapter's 10 kΩ, B = 3950 thermistor while its nominal point stays at 25 °C.
ObserveAt 47.2 °C, the ideal Beta curve is about 4.00 kΩ and −3.85%/K. At 25 °C the slope was −4.44%/K, so its magnitude has dropped about 13.4%.
ExplainThe curve flattens because temperature appears squared in the slope denominator. A constant B shapes a changing slope; it does not make sensitivity constant.
The resistance conversion fixes Beta at 3950 K and the reference at 10 kohm and 25 C. It leaves out self-heating, lead resistance, divider loading, tolerance, ageing, converter error, and lot variation, and does not replace fitted coefficients or measured reference checks.
- Steinhart-Hart coefficients
- Needs separate evidence
- measured reference points
- Needs separate evidence
Use field evidence or a deeper model before release.
5. Recover the hidden energy
This makes the datasheet constant checkable as a material-scale energy rather than a magic firmware number.
6. Decide where the fit is safe
Use the Beta curve near the range where its coefficients were validated. If residuals grow across a wide span, record them and move to a richer fit instead of pretending the local model is complete.
7. Check yourself
Why must temperature be in kelvin?
Why does sensitivity magnitude fall when temperature rises?
Does 0.340 eV prove every B = 3950 thermistor is identical?
The resistance conversion fixes Beta at 3950 K and the reference at 10 kohm and 25 C. It leaves out self-heating, lead resistance, divider loading, tolerance, ageing, converter error, and lot variation, and does not replace fitted coefficients or measured reference checks.
- the chapter's B = 3950 K
- Thermistor Beta temperature parameter
- R0 = 10 kΩ at 25 °C
- Thermistor reference resistance and temperature
- 47.2 °C point
- Temperature calculated at four-kilohm resistance
- Boltzmann conversion
- Beta converted to activation energy using Boltzmann constant
Results describe the stated ideal Beta law, not a complete thermistor calibration certificate.
Phoebe guides