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 \( \epsilon_0 = 9 \times 10^{-12} \, \text{C}^2/\text{Nm}^2 \))
Remember Gauss’s law and the formula for electric flux. Pay close attention to the direction of the electric field and the area vector when calculating the flux.
The problem involves finding the charge enclosed in a cube using Gauss's Law, which states: \(\Phi_E = \frac{Q_{\text{enclosed}}}{\epsilon_0}\). Here, \(\Phi_E\) is the electric flux through the cube, and \(Q_{\text{enclosed}}\) is the charge we need to find.
The electric field is given by: \(\vec{E} = E_0 x \hat{i}\) where \(E_0 = 4 \times 10^4 \, \text{NC}^{-1} \, \text{m}^{-1}\).
Convert \(a\) from cm to meters: \(a = 2\,\text{cm} = 0.02\,\text{m}\).
The electric flux through a face parallel to the yz-plane (at \(x=a\)) is:
\(\Phi_E = \int \vec{E} \cdot d\vec{A} = \int_{0}^{a} E_0 x \cdot a^2 \, dy \, dz = E_0 \cdot a \cdot a^2 = E_0 a^3\).
Since \(\vec{E}\) is zero at \(x=0\) face and across the other faces (where it is perpendicular), the total flux is determined solely by the face at \(x = a\):
\(\Phi_E = E_0 a^3 = 4 \times 10^4 \times (0.02)^3 \, \text{Nm}^2/\text{C} = 32 \times 10^{-6} \, \text{Nm}^2/\text{C}\).
Using Gauss's Law, we have:
\(\Phi_E = \frac{Q_{\text{enclosed}}}{\epsilon_0} \Rightarrow Q_{\text{enclosed}} = \Phi_E \cdot \epsilon_0\).
Calculating \(Q_{\text{enclosed}}\):
\(Q_{\text{enclosed}} = 32 \times 10^{-6} \cdot 9 \times 10^{-12} \, \text{C} = 288 \times 10^{-18} \, \text{C}\).
Express \(Q_{\text{enclosed}}\) in terms of \(Q\):
\(Q_{\text{enclosed}} = Q \times 10^{-14} \Rightarrow Q = \frac{288 \times 10^{-18}}{10^{-14}} = 288\).
Thus, the value of \(Q\) is 288, fitting perfectly within the provided range (288,288).
