A capacitive transducer works on the principle of change in capacitance due to a change in the physical quantity being measured. The capacitance ($C$) of a parallel plate capacitor is given by the formula: $$ C = \frac{\epsilon A}{d} $$ where:
- $C$ is the capacitance
- $\epsilon$ is the permittivity of the dielectric material between the plates
- $A$ is the area of overlap of the plates
- $d$ is the distance between the plates
When a capacitive transducer measures displacement by varying the distance ($d$) between the plates, the relationship between capacitance and displacement is inverse: $C \propto \frac{1}{d}$. This inverse relationship means that the output (capacitance) is not directly proportional to the input (displacement). Therefore, the behavior is inherently non-linear.
- (A) Linear behaviour: This would imply a direct proportionality, which is not the case for capacitance varying with distance.
- (B) Non-linear behaviour: As explained by the inverse relationship, this is the correct description.
- (C) Like y = 2x curve: This represents a linear relationship, which is incorrect.
- (D) Like y = mx+b curve: This also represents a linear relationship, which is incorrect.
While some linearization techniques can be applied in practice (e.g., using a differential capacitive transducer), the fundamental behavior of a single capacitive transducer with varying distance is non-linear.