The correct answer is:
(d) v=−ΔR×Vdc2×(2R+ΔR)v = -\frac{\Delta R \times V_{\text{dc}}}{2 \times (2R + \Delta R)}v=−2×(2R+ΔR)ΔR×Vdc
Explanation:
A transducer bridge typically uses resistors in a Wheatstone bridge configuration to measure changes in resistance (ΔR\Delta RΔR) caused by a physical parameter such as pressure, temperature, or strain. The output voltage vvv is derived based on the following assumptions:
- All resistors initially have the same resistance RRR, and one or more resistors change by a small amount ΔR\Delta RΔR.
- VdcV_{\text{dc}}Vdc is the supply voltage applied to the bridge.
The general equation for the output voltage vvv of a transducer bridge, taking into account a small change in resistance, is given as:
v=−ΔR×Vdc2×(2R+ΔR)v = -\frac{\Delta R \times V_{\text{dc}}}{2 \times (2R + \Delta R)}v=−2×(2R+ΔR)ΔR×Vdc
This equation accurately reflects the relationship between the resistance change (ΔR\Delta RΔR), the DC supply voltage (VdcV_{\text{dc}}Vdc), and the output voltage vvv.