The electric flux (Φ) through a closed surface such as a cube can be calculated using Gauss's law: \( Φ = \oint \vec{E} \cdot d\vec{A} \), where \( \vec{E} \) is the electric field, and \( d\vec{A} \) is the differential area vector. Given the electric field \( \vec{E} = (2x \hat{i}) \, \text{N C}^{-1} \), the flux through surfaces perpendicular to other axes will be zero because the field is only in the x-direction.
Consider the cube positioned from \( x = 0 \) to \( x = 2 \) with side length \( a = 2 \, \text{m} \). The cube has two faces perpendicular to the x-axis at \( x = 0 \) and \( x = 2 \). The area \( A \) of each face is \( A = 2 \times 2 = 4 \, \text{m}^2 \).
For the face at \( x = 0 \):
\( \vec{E} = 2(0) \hat{i} = 0 \) so flux, \( Φ_0 = E \cdot A = 0 \times 4 = 0 \, \text{N m}^2/\text{C} \).
For the face at \( x = 2 \):
\( \vec{E} = 2(2) \hat{i} = 4 \, \text{N C}^{-1} \) and outward \( d\vec{A} = 4 \hat{i} \), so flux, \( Φ_2 = E \cdot A = 4 \times 4 = 16 \, \text{N m}^2/\text{C} \).
The total flux through the cube is \( Φ_{\text{total}} = Φ_0 + Φ_2 = 0 + 16 = 16 \, \text{N m}^2/\text{C} \).
The computed value \( 16 \, \text{N m}^2/\text{C} \) falls within the expected range of (16,16).
The electric flux is given by Gauss's Law:
\(\Phi = \oint \vec{E} \cdot d\vec{A}.\)
The field $\vec{E} = 2x \hat{i}$ varies with $x$.
For the cube, only the left ($x = 0$) and right ($x = 2$) faces contribute: \(\Phi = E_\text{right} A - E_\text{left} A.\)
Substituting $A = 4 \, \mathrm{m}^2$, $E_\text{right} = 2(2) = 4$, and $E_\text{left} = 2(0) = 0$:
\(\Phi = 4 \cdot 4 - 0 \cdot 4 = 16 \, \mathrm{Nm}^2/\mathrm{C}.\)
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,


| LIST I | LIST II | ||
| A | Gauss's Law in Electrostatics | I | \(\oint \vec{E} \cdot d \vec{l}=-\frac{d \phi_B}{d t}\) |
| B | Faraday's Law | II | \(\oint \vec{B} \cdot d \vec{A}=0\) |
| C | Gauss's Law in Magnetism | III | \(\oint \vec{B} \cdot d \vec{l}=\mu_0 i_c+\mu_0 \in_0 \frac{d \phi_E}{d t}\) |
| D | Ampere-Maxwell Law | IV | \(\oint \vec{E} \cdot d \vec{s}=\frac{q}{\epsilon_0}\) |
A cubical volume is bounded by the surfaces \( x = 0 \), \( x = a \), \( y = 0 \), \( y = a \), \( z = 0 \), \( z = a \). The electric field in the region is given by: \[ \vec{E} = E_0 x \hat{i} \]
Where \( E_0 = 4 \times 10^4 \, \text{NC}^{-1} \, \text{m}^{-1} \). If \( a = 2 \, \text{cm} \), the charge contained in the cubical volume is \( Q \times 10^{-14} \, \text{C} \). The value of \( Q \) is ______. (Take \( \epsilon_0 = 9 \times 10^{-12} \, \text{C}^2/\text{Nm}^2 \))

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 : \(A_2 \rightleftharpoons 2A\)