Step 1: The equation of state is given by the relation: \[ P T^3 = {constant}. \] This indicates that the product of the pressure \( P \) and the cube of the temperature \( T \) remains constant during the expansion.
Step 2: The coefficient of volume expansion \( \beta \) is defined as: \[ \beta = \frac{1}{V} \left( \frac{\Delta V}{\Delta T} \right)_P, \] which can be related to the change in temperature under constant pressure.
Step 3: To relate the volume expansion to the temperature, we differentiate the given equation \( P T^3 = {constant} \). Differentiating with respect to \( T \) gives: \[ P \cdot 3T^2 \cdot \frac{dT}{dT} + T^3 \cdot \frac{dP}{dT} = 0 \quad \Rightarrow \quad \frac{dP}{dT} = -\frac{3P}{T}. \]
Step 4: The relationship for the volume change is now obtained by considering that: \[ \frac{dV}{V} = \beta \, dT \quad \Rightarrow \quad \beta = \frac{4}{T}. \]
Step 5: Hence, the coefficient of volume expansion is \( \beta = \frac{4}{T} \).
Define the current gain \( \alpha_{DC} \) and \( \beta_{DC} \) for a transistor. Obtain the relation between them.
Equipotential surfaces are shown in the figure. The electric field strength will be: