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 black body is at a temperature of 2880 K. The energy of radiation emitted by this body with wavelength between 499 nm and 500 nm is U1, between 999 nm and 1000 nm is U2 and between 1499 nm and 1500 nm is U3. The Wien's constant, b = 2.88×106 nm-K. Then,


What will be the equilibrium constant of the given reaction carried out in a \(5 \,L\) vessel and having equilibrium amounts of \(A_2\) and \(A\) as \(0.5\) mole and \(2 \times 10^{-6}\) mole respectively?
The reaction : \(A_2 \rightleftharpoons 2A\)