To find the area of the rectangular surface, we start with the formula for electric flux: \( \Phi = \vec{E} \cdot \vec{A} \). Here, the electric field \( \vec{E} \) is given by: \( \vec{E} = (2\hat{i} + 4\hat{j} + 6\hat{k}) \times 10^3 \, N/C \). The flux \( \Phi \) is given as \( 6.0 \, Nm^2C^{-1} \).
The surface is parallel to the x-z plane. For a surface parallel to the x-z plane, the area vector \( \vec{A} \) is perpendicular to the plane in the y-direction and can be expressed as \( \vec{A} = A\hat{j} \).
Since only the j-component of \( \vec{E} \) contributes to the flux, we have: \( \Phi = E_y \cdot A \), where \( E_y = 4 \times 10^3 \, N/C \).
Substituting the values, \( 6.0 = 4 \times 10^3 \times A \).
Solving for \( A \): \( A = \frac{6.0}{4 \times 10^3} = 1.5 \times 10^{-3} \, m^2 \).
Convert the area to \( cm^2 \): \( A = 1.5 \times 10^{-3} \, m^2 \times (10^4 \, cm^2/m^2) = 15 \, cm^2 \).
The area of the surface is 15 \( cm^2 \), which falls within the given range of 15,15, thus confirming the solution.
A small bob of mass 100 mg and charge +10 µC is connected to an insulating string of length 1 m. It is brought near to an infinitely long non-conducting sheet of charge density \( \sigma \) as shown in figure. If the string subtends an angle of 45° with the sheet at equilibrium, the charge density of sheet will be : 
A point charge $ +q $ is placed at the origin. A second point charge $ +9q $ is placed at $ (d, 0, 0) $ in Cartesian coordinate system. The point in between them where the electric field vanishes is:
The molar mass of the water insoluble product formed from the fusion of chromite ore \(FeCr_2\text{O}_4\) with \(Na_2\text{CO}_3\) in presence of \(O_2\) is ....... g mol\(^{-1}\):
Given below are some nitrogen containing compounds:
Each of them is treated with HCl separately. 1.0 g of the most basic compound will consume ...... mg of HCl.
(Given Molar mass in g mol\(^{-1}\): C = 12, H = 1, O = 16, Cl = 35.5.)
