Calibration of a Temperature Sensor

Introduction:

Thermometry is the measurement of the temperature of an object or system. Our skin has a sense of temperature, but it is not very reliable. After exposure to a given temperature for a sufficient amount of time our skin (or our brain) tends to have that temperature feel normal. Any physical property that varies with temperature (which is almost ALL physical properties) can be used as thermometers. It is desirable to have a nice, linear behavior of the thermometric property on the temperature. In many cases this is not possible, unless one is willing to change thermometers often. In the upcoming labs we will be using conventional liquid-in-glass thermometers and electronic temperature sensors. Today we will confirm the inappropriateness of using our sense of temperature for quantitative (or even qualitative) measurements and investigate how to calibrate an uncalibrated electronic temperature sensor to make useful measurements.

 

Response of the Skin to Objects of Different Temperature

There will be three pans of water located in the lab. One will be a mixture of ice and water and its temperature will be about 32 °F or 0 °C. There will be another pan of water at a temperature much warmer than room temperature – around 100 °F. The third pan will be at room temperature. Each will have thermometers so that you can accurately determine the true temperature. Place one hand in the hot water and the other in the ice water for about 20 seconds. Then place both hands into the room temperature water. Comment on the temperature sensed by each hand.

 

Calibration of an Electronic Temperature Sensor

There are many kinds of thermometers.  Some are more familiar than others - liquid-in-glass being the most common type.  The LabPro that we used frequently last semester can be equipped with a sensor that measures changes in temperature - i.e., a temperature probe.  The probes can be calibrated directly in temperature, but we will prefer to use the uncalibrated data to learn how the raw data (a voltage) is turned into a useful temperature value.

Experimental steps:

V = B + M*T

            where M is the slope of the line and B is the y-intercept.