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 $E_\text{left} = 2(0) = 0$:
\(\Phi = 4 \cdot 4 - 0 \cdot 4 = 16 \, \mathrm{Nm}^2/\mathrm{C}.\)

| 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 | \(\oint \vec{E} \cdot d \vec{s}=\frac{q}{\epsilon_0}\) |

Let \( f : \mathbb{R} \to \mathbb{R} \) be a twice differentiable function such that \[ (\sin x \cos y)(f(2x + 2y) - f(2x - 2y)) = (\cos x \sin y)(f(2x + 2y) + f(2x - 2y)), \] for all \( x, y \in \mathbb{R}. \)
If \( f'(0) = \frac{1}{2} \), then the value of \( 24f''\left( \frac{5\pi}{3} \right) \) is: