The two terminals are used to supply the Us bridge circuit. The voltage Us is also called excitation voltage or excitation voltage or sensor input.
Usually the bridge circuit with DC voltage of 5V is supplied. Are also common 2.5V bridge supply or 1.0V bridge supply if, for example, a low strain gauges is (DMS) with 120 Ohm used, or if the DMS is bonded to a non-conductive material, so that a strong self-heating of the strain gage must be prevented.
About the two other terminals Ud is the voltage at the output of the DMS measured.
The voltage Ud is called "differential voltage" or "bridge output" or "sensor output".
The relationship between the bridge output Ud and the resistance change ΔR/R is for the full-bridge:
Ud / Us = 1/4 (¨R1 / R1 - ΔR2 / R2 + ΔR3 / R3 - ΔR4 / R4) (Equation 1)
ΔR/R: relative change in resistance
Ud / Us: relative bridge output
Derivation of the equation for the bridge circuit: Wheatstone bridge.pdf
The relative bridge output Ud/Us is usually less than 0.1%. At 5V bridge excitation voltages Ud therefore must be measured from -0.5 to +0.5 mV. Therefore, a sense amplifier is used.
The amplifier has several functions:
By standardizing the bridge output Ud on the supply voltage Us, the display values on measuring amplifiers with different supply voltage Us directly comparable. The default setting of the unit on the display of many measuring amplifier is therefore mV/V.
The relationship between bridge output, supply voltage and strain follows from equations (1) and (2):
Ud/Us = 1/4 k (ε1 - ε2 + ε3 - ε4) (Equation 3)
For one quarter bridge is due ε2 = ε3 = ε4 = 0:
From equation (4) gives the relationship between display Ud / Us and strain ε for a quarter bridge:
ε1 = Ud/Us 4/k (Equation 5)
In a k-factor of 2.0 an indication Ud/Us of 2.0 mV/V (= 0.002 V/V = 2.0E-3) means:
0.002 x 4/2.0 = ε1 = 0.004 = 4 ‰ = 4000 µm/m
2 mV/V therefore correspond to 4000 µm/m strain at a quarter bridge with k-factor. 2
The bridge circuit allows the determination of very small changes in resistance.
At the same temperature-induced changes in resistance and other interference are compensated for.
However, a prerequisite for a good compensation of interferences that the disorder equally affecting two adjacent resistors of the bridge circuit.
The relationship between resistance change ΔR/R and strain ε is defined by the k-factor of the strain gauge.
If the elongation of an electrical conductor, a change in cross section of the electrical conductor to the sequence. The change in cross section of the electrical conductor is in turn connected to a change in electrical resistance.
From the condition that an "elongation" (positive elongation) of a conductor in volume still remains constant, resulting in a "necking" of the conductor. Conversely, results from an "upsetting" (negative strain) a "thickening" of the conductor.
This, purely geometrical effect results under the condition constant conductor volume to a linear relationship between resistance change and expansion:
ΔR1/R1 = k ε (Equation 2)
The Propotionalitätsfaktor is referred to as k-factor of the strain gauge. For alloys whose volume remains constant while stretching (and this applies to all electrical conductor) results in a k-factor of 2.
1 ‰ elongation corresponds to 2 ‰ change in resistance, or
1000 .mu.m / m elongation corresponding 2 ‰ change in resistance, or
1000 e 6 strain corresponding 2000 E-6 resistance change