A hollow cylinder has a charge q coulomb within it. It ϕ is the electric flux associated with the curved surface B, the flux linked with the plane surface A will be
\(\frac {ϕ}{3}\)
\(\frac {q}{ε_0} - ϕ\)
\(\frac {1}{2}(\frac {q}{ε_0} - Φ)\)
Zero
The flux linked with a closed surface is given by Gauss's Law.
Φ = \(\frac {q}{ε₀}\)
In the given scenario, there is a charge q within the hollow cylinder. Let's consider the curved surface B and the plane surface A separately.
For the curved surface B, the electric flux associated with it is ϕ.
For the plane surface A, the flux linked with it can be calculated as follows:
Φ(A) = Φ - Φ(B)
Substituting the values, we get:
Φ(A) = \(\frac {q}{ε₀}\) - ϕ
Therefore, the correct answer is (C) \(\frac {1}{2}(\frac {q}{ε_0} - Φ)\).
The magnitude of heat exchanged by a system for the given cyclic process ABC (as shown in the figure) is (in SI units):
Gauss law states that the total amount of electric flux passing through any closed surface is directly proportional to the enclosed electric charge.
According to the Gauss law, the total flux linked with a closed surface is 1/ε0 times the charge enclosed by the closed surface.
For example, a point charge q is placed inside a cube of edge ‘a’. Now as per Gauss law, the flux through each face of the cube is q/6ε0.
As per the Gauss theorem, the total charge enclosed in a closed surface is proportional to the total flux enclosed by the surface. Therefore, if ϕ is total flux and ϵ0 is electric constant, the total electric charge Q enclosed by the surface is;
Q = ϕ ϵ0
The Gauss law formula is expressed by;
ϕ = Q/ϵ0
Where,
Q = total charge within the given surface,
ε0 = the electric constant.