The line integral of the electric field along a path is related to the change in electric potential \( V \) between the start and end points of the path. Mathematically:
\[ \oint_{\mathcal{C}} \mathbf{E} \cdot d\mathbf{l} = V_C - V_M \]
where:
The electric potential due to a point charge \( q \) at a distance \( r \) is given by:
\[ V = \frac{kq}{r} \]
where \( k \) is Coulombβs constant.
Both points \( C \) and \( M \) are at the same distance \( 2d \) from the charges \( Q \) (at A) and \( 2Q \) (at B), since \( MCL \) is a semicircle of radius \( 2d \). Therefore, the electric potential at both \( C \) and \( M \) is the same.
For any point on the semicircle:
\[ V = \frac{kQ}{2d} + \frac{k(2Q)}{2d} = \frac{3kQ}{2d} \]
Thus,
\[ V_C = V_M \]
Since the potentials at points \( C \) and \( M \) are equal (\( V_C = V_M \)):
\[ \oint_{\mathcal{C}} \mathbf{E} \cdot d\mathbf{l} = V_C - V_M = 0 \]
The line integral of the electric field along the given path is zero.
The P-V diagram of an engine is shown in the figure below. The temperatures at points 1, 2, 3 and 4 are T1, T2, T3 and T4, respectively. 1β2 and 3β4 are adiabatic processes, and 2β3 and 4β1 are isochoric processes
Identify the correct statement(s).
[Ξ³ is the ratio of specific heats Cp (at constant P) and Cv (at constant V)]