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Technical Notes

Thermistor Definition

The world thermistor is derived from its description: “Thermal sensitive resistor”. Thermistors are passive semiconductors, which produce resistance

values dependent on temperature.

 

A Negative Temperature Coefficient (NTC) thermistor decreases in resistance as its body temperature increases. In fact, NTC thermistors exhibit two characteristics, which make them extremely useful in a variety of applications. Their change in resistance is predicable and its is relatively large per degree change in temperature.

Manufacturing Process

This is a two-step process of chip manufacturing and thermistor assembly. Metal oxide powders into ceramic sheets process manufactured chips. These sheets are moralized with silver to allow for electrical contact. After moralization, the ceramic sheets are diced into chips. Each chip is tested to meet our superior quality standards.

After a chip has been manufactured and tested, leads are attached. The chip is trimmed to match the specified tolerance, and then a protective coating is added. Adding housings, cables and connectors can do further customizing of the assembly.

Thermistor quality is assured with in-process inspection and Statistical Process Control (SPC). This process takes place at each manufacturing and assembly step. All Finished products are 100% tested both electrically and mechanically to guarantee all specifications are met.

Resistance-Temperature(R/T) Curves and Negative Temperature Coefficient

Nine different materials are made, each with its own unique and predictable resistance-temperature characteristics. These characteristics are called “curves”. Thermistors are most often specified by their curve and by their resistance value at 25.

The NTC (Negative Temperature Coefficient) is the negative percent resistance change per degree C. Our thermistors have NTC values at 25°C ranging from –3.9% to –6.4%. Resistance values at 25 range from 300 ohms to 40 meg ohms. The tables on pages 23 through 25 detail this information.

Thermal Time Constant

Time constant, expressed in seconds, is the time required for a thermistor to indicate 63.2% of a newly impressed temperature. The time constant of a thermistor is directly affected by the mass of the thermistor and thermal coupling to the environment. An epoxy or phenolic coated thermistor coupling to the environment. An epoxy or phenolic coated thermistor with a 0.095” O.D. will typical have a time constant of 0.75 seconds in stirred oil and 10 seconds in still air.

Dissipation Constant

Dissipation constant is the power required to raise the temperature of a thermistor 1 above the surrounding environment. Power is expressed in watts. The dissipation constant of a thermistor with a 0.095” O.D., coated with epoxy or phenolic, is typically 13 mW/ in stirred oil and 2 mW/ in still air.

Voltage/Current Requirements

Very low current is required for a thermistor being used in temperature measurement, control or compensation applications. Current levels should typically be less than 100mA for a thermistor to dissipate “zero power”. As previously discussed, power dissipation for a thermistor in still air is approximately 2mW/. Therefore, in order to keep the thermal error (self-heat) below 0.1, the power dissipation must be less than 0.2mW.

Self-heating is desirable in applications such as airflow measurement and liquid level control. Standard epoxy or phenolic coated thermistors with a 0.095” O.D. have a maximum power rating of 30 milliwatts at 25 to 1 milliwatt at 100.

Beta

The Beta value of a thermistor is one way to characterize its resistance temperature relationship. Beta is calculated as follows:

βT2 / T1 = ζn(RT2/RT1)/(1/T2 – 1/T1)

Temperature is in degrees Kelvin; RT1 is the resistance at temperature T1; RT2 is the resistance at temperature T2.

Steinhart-Hart Equation

The Steinhart-hart Equation is an empirically developed polynomial, which best represents the resistance temperature relationships of NTC thermistors. The Steinhart-Hart Equation is more accurate than previously methods; as well, it is more accurate over wider temperature ranges. To solve for temperature when resistance is known, the form of the equation is:

1/T=a+b(ζnR)+c(ζnR)3

To solve for resistance when temperature is known, the form of the equation is:

R=e(exp)[(-α/2+(α2/4+α3/27)-2)-3+(-α/2-(α2/4+α3/27)2)3]

Where alpha = (a-1/T)c and β = b/c

For both forms of the equation T is temperature expressed in degrees Kelvin; a, b and c can be solved simultaneously using the following:

1/T1=a+b(ζnR1)+c(ζnR1)3

1/T2=a+b(ζnR2)+c(ζnR2)3

1/T3=a+b(ζnR3)+c(ζnR3)3

The data calculated by these equations will be accurate to better than +0.01 when -40 is less than or equal to 150 and T1-T2 is less than or equal to 50 and T2-T3 is less than or equal to 50 and T1, T2 and T3 are evenly spaced.

Maximum Temperature Rating/ Recommended Operating Ranges

Our thermistors may be intermittently cycled at temperatures from -50 to 150. Stability is achieved when the thermistors are  stored at temperatures less than 50 and operated continuously at temperatures less than 100. For interchangeable thermistors, optimum stability is achieved when the thermistors are operated at temperatures within the specified interchangeable temperature range.

Stability

Years of experience in thermistor manufacturing, coupled with stringent process controls, ensure that highly stable thermistors are produced. In fact, our thermistors typically exhibit less than 0.02 thermometric drift per year when stored or operated at temperatures less than 50. The stability of a thermistor is greatly dependent on environmental conditions such as humidity, excessive temperatures and thermal shock; these effects should be minimized to guarantee stability.

OCTSENS TECH CO., LTD.

4F., No. 22, Ln 75, Sec. 2, Jhongjua Rd.,

Jhongjheng Dist., Taipei City 10065, Taiwan, R.O.C.

Tel: 886-2-23883573    Fax: 886-2-23883575

E-mail: sales@octsensors.com    www.octsensors.com