Given: - \( C_1 \) encloses charge \( 2Q \) - \( C_2 \) encloses charge \( 3Q \)
According to Gauss’s law, the electric flux \( \Phi \) through a closed surface is given by:
\[ \Phi = \frac{q_{\text{enc}}}{\varepsilon_0} \] where \( q_{\text{enc}} \) is the total charge enclosed by the surface and \( \varepsilon_0 \) is the permittivity of free space.
The charge enclosed by \( C_1 \) is \( 2Q \). Therefore, the electric flux through \( C_1 \) is:
\[ \Phi_{C_1} = \frac{2Q}{\varepsilon_0} \]
The charge enclosed by \( C_2 \) is \( 3Q \). Therefore, the electric flux through \( C_2 \) is:
\[ \Phi_{C_2} = \frac{3Q}{\varepsilon_0} \]
The ratio of the electric flux passing through \( C_1 \) and \( C_2 \) is given by:
\[ \text{Ratio} = \frac{\Phi_{C_1}}{\Phi_{C_2}} = \frac{\frac{2Q}{\varepsilon_0}}{\frac{3Q}{\varepsilon_0}} = \frac{2}{3} \]
However, the question asks for the inverse ratio (flux ratio through \( C_2 \) to \( C_1 \)), which simplifies to:
\[ \text{Ratio} = \frac{3}{2} \]
The ratio of electric flux passing through \( C_1 \) and \( C_2 \) is \( 2 : 5 \).
A square loop of sides \( a = 1 \, {m} \) is held normally in front of a point charge \( q = 1 \, {C} \). The flux of the electric field through the shaded region is \( \frac{5}{p} \times \frac{1}{\varepsilon_0} \, {Nm}^2/{C} \), where the value of \( p \) is:
Let \[ I(x) = \int \frac{dx}{(x-11)^{\frac{11}{13}} (x+15)^{\frac{15}{13}}} \] If \[ I(37) - I(24) = \frac{1}{4} \left( b^{\frac{1}{13}} - c^{\frac{1}{13}} \right) \] where \( b, c \in \mathbb{N} \), then \[ 3(b + c) \] is equal to:
For the thermal decomposition of \( N_2O_5(g) \) at constant volume, the following table can be formed, for the reaction mentioned below: \[ 2 N_2O_5(g) \rightarrow 2 N_2O_4(g) + O_2(g) \] Given: Rate constant for the reaction is \( 4.606 \times 10^{-2} \text{ s}^{-1} \).