Chapter 8 Tutorial

Measurement Fundamentals

y

I bdM ys q °uysq””

 

”q xqwu uqsu y q sxq y °uqu y q

 

usyu” “4 dxu yq”

MWW °uqu u uqsu v

bdM q q”s”q yq”uuu4

 

 

I bdM xq u xywxuqry”yv °uqu qsu

 

dxu v q

bdM yu

bdM q w

sxysu v xywx3qssqsw3u° °uqu°uxu RZ 9:A=6I

 

bdM x

α E 64669>; .MSX 5 SNL =;7/ qt

α E 64669A74

“PT100” is a special label that is sometimes used to refer to an bdM with α = 0.00385 and R6 = 100Ω.

The resistance of an bdM is nominal at 0 °C and is referred to as R6. The HP 34970A can measure bdMs with R6 values from 49Ω to 2.1 kΩ.

You can measure bdMs using a 2-wire or 4-wire measurement method. The 4-wire method (with offset compensation) provides the most accurate way to measure small resistances. Connection lead resistance is automatically removed using the 4-wire method.

A thermistor is constructed of materials

that non-linearly changes resistance with changes in temperature. The internal MWW measures the resistance of the thermistor and then calculates the equivalent temperature.

Thermistors have a higher sensitivity than thermocouples or bdMs. This makes a thermistor a good choice when measuring very small changes in temperature. Thermistors are, however, very non-linear, especially at high temperatures and function best below 100 °C.

Because of their high resistance, thermistors can be measured using a 2-wire measurement method. The internal MWW supports

2.2 kΩ (44004), 5 kΩ (44007), and 10 kΩ (44006) thermistors.

346

Page 342
Image 342
HP 34970A manual Measurement Fundamentals