Given data:
Using Gauss's Law, the total electric flux through the Gaussian surface is equal to the total charge enclosed divided by the permittivity of free space:
\(\Phi = \frac{Q_{\text{enc}}}{\epsilon_0}\)
The electric flux through a surface is given by:
\(\Phi = E \cdot A \cdot \cos(\theta)\)
Since the electric field lines are parallel to the x-axis, the angle \( \theta \) between the electric field and the normal to the surfaces ABCD and EFGH is \( 0^\circ \) and \( 180^\circ \) respectively. Therefore, \( \cos(0^\circ) = 1 \) and \( \cos(180^\circ) = -1 \).
The area of each face of the cube is:
\(A = a^2 = (0.1 \, \text{m})^2 = 0.01 \, \text{m}^2\)
The electric flux through surface ABCD is:
\(\Phi_{ABCD} = E_{ABCD} \cdot A \cdot \cos(0^\circ) = 6 \times 10^3 \, \text{N/C} \cdot 0.01 \, \text{m}^2 \cdot 1 = 60 \, \text{N} \cdot \text{m}^2/\text{C}\)
The electric flux through surface EFGH is:
\(\Phi_{EFGH} = E_{EFGH} \cdot A \cdot \cos(180^\circ) = 9 \times 10^3 \, \text{N/C} \cdot 0.01 \, \text{m}^2 \cdot (-1) = -90 \, \text{N} \cdot \text{m}^2/\text{C}\)
The total electric flux through the Gaussian surface is the sum of the fluxes through all surfaces. Since the electric field lines are parallel to the x-axis, the flux through the other four faces is zero. Therefore, the total flux is:
\(\Phi_{\text{total}} = \Phi_{ABCD} + \Phi_{EFGH} = 60 \, \text{N} \cdot \text{m}^2/\text{C} + (-90 \, \text{N} \cdot \text{m}^2/\text{C}) = -30 \, \text{N} \cdot \text{m}^2/\text{C}\)
Using Gauss's Law, the total charge enclosed by the cube is:
\(Q_{\text{enc}} = \Phi_{\text{total}} \cdot \epsilon_0 = -30 \, \text{N} \cdot \text{m}^2/\text{C} \cdot 9 \times 10^{-12} \, \text{F/m}\)
\(Q_{\text{enc}} = -270 \times 10^{-12} \, \text{C} = -0.27 \times 10^{-9} \, \text{C} = -0.27 \, \text{nC}\)
Therefore, the total charge enclosed by the cube is \( \boxed{-0.27 \, \text{nC}} \).
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 \( \epsilon_0 = 9 \times 10^{-12} \, \text{C}^2/\text{Nm}^2 \))