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The electric field in a region of space ...

The electric field in a region of space varies as `E=(xhati+2yhatj)+3zhatk)` V/m
(a). Consider an elemental cuboid whose one vertex is at (x,y,z) and the three sides are dx, dy and dz, sides being parallel to the three co-ordinate axes. Calculate the flux of electric field through the cube.
(b). Usig the expression obtained in (a) find the charge enclosed by a spherical surface of radius r, centred at the origin.

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To solve the problem step by step, we will address both parts (a) and (b) of the question. ### Part (a): Calculate the flux of the electric field through the cube. 1. **Identify the Electric Field**: The electric field is given by: \[ \mathbf{E} = (x \hat{i} + 2y \hat{j} + 3z \hat{k}) \, \text{V/m} \] 2. **Define the Elemental Cuboid**: Consider an elemental cuboid with one vertex at \((x, y, z)\) and dimensions \(dx\), \(dy\), and \(dz\). 3. **Calculate the Flux through Each Face of the Cuboid**: The electric flux \(\Phi\) through a surface is given by: \[ \Phi = \int \mathbf{E} \cdot d\mathbf{A} \] where \(d\mathbf{A}\) is the area vector of the surface. - **Face 1 (x = constant)**: Area vector \(d\mathbf{A} = dy \, dz \hat{i}\) \[ \Phi_1 = \mathbf{E} \cdot d\mathbf{A} = (x \hat{i} + 2y \hat{j} + 3z \hat{k}) \cdot (dy \, dz \hat{i}) = x \, dy \, dz \] - **Face 2 (x + dx = constant)**: Area vector \(d\mathbf{A} = -dy \, dz \hat{i}\) \[ \Phi_2 = -\mathbf{E} \cdot d\mathbf{A} = -(x + dx)(dy \, dz) = -(x \, dy \, dz + dx \, dy \, dz) \] - **Face 3 (y = constant)**: Area vector \(d\mathbf{A} = dx \, dz \hat{j}\) \[ \Phi_3 = (x \hat{i} + 2y \hat{j} + 3z \hat{k}) \cdot (dx \, dz \hat{j}) = 2y \, dx \, dz \] - **Face 4 (y + dy = constant)**: Area vector \(d\mathbf{A} = -dx \, dz \hat{j}\) \[ \Phi_4 = -\mathbf{E} \cdot d\mathbf{A} = -(x \hat{i} + 2(y + dy) \hat{j} + 3z \hat{k}) \cdot (-dx \, dz \hat{j}) = -2(y + dy) \, dx \, dz \] - **Face 5 (z = constant)**: Area vector \(d\mathbf{A} = dx \, dy \hat{k}\) \[ \Phi_5 = (x \hat{i} + 2y \hat{j} + 3z \hat{k}) \cdot (dx \, dy \hat{k}) = 3z \, dx \, dy \] - **Face 6 (z + dz = constant)**: Area vector \(d\mathbf{A} = -dx \, dy \hat{k}\) \[ \Phi_6 = -\mathbf{E} \cdot d\mathbf{A} = -(x \hat{i} + 2y \hat{j} + 3(z + dz) \hat{k}) \cdot (-dx \, dy \hat{k}) = -3(z + dz) \, dx \, dy \] 4. **Total Flux Calculation**: Now, summing all the flux contributions: \[ \Phi = \Phi_1 + \Phi_2 + \Phi_3 + \Phi_4 + \Phi_5 + \Phi_6 \] \[ \Phi = (x \, dy \, dz - (x \, dy \, dz + dx \, dy \, dz) + 2y \, dx \, dz - 2(y + dy) \, dx \, dz + 3z \, dx \, dy - 3(z + dz) \, dx \, dy) \] Simplifying this expression leads to: \[ \Phi = 6 \, dx \, dy \, dz \] ### Part (b): Find the charge enclosed by a spherical surface of radius \(r\) centered at the origin. 1. **Use Gauss's Law**: Gauss's law states: \[ \Phi = \frac{Q_{\text{enc}}}{\epsilon_0} \] where \(Q_{\text{enc}}\) is the charge enclosed and \(\epsilon_0\) is the permittivity of free space. 2. **Substituting the Flux**: From part (a), we found that the flux through the cuboid is: \[ \Phi = 6 \, dx \, dy \, dz \] 3. **Volume Element**: The volume element \(dV\) of the cuboid is: \[ dV = dx \, dy \, dz \] 4. **Charge Density**: The charge density \(\rho\) can be expressed as: \[ \rho = \frac{Q_{\text{enc}}}{dV} = 6 \epsilon_0 \] 5. **Total Charge Enclosed in a Sphere**: The total charge enclosed by a sphere of radius \(r\) is: \[ Q_{\text{enc}} = \rho \cdot V = 6 \epsilon_0 \cdot \frac{4}{3} \pi r^3 \] Therefore, \[ Q_{\text{enc}} = 8 \epsilon_0 \pi r^3 \] ### Final Answers: - **(a)** The flux of the electric field through the cuboid is \(6 \, dx \, dy \, dz\). - **(b)** The charge enclosed by a spherical surface of radius \(r\) is \(8 \epsilon_0 \pi r^3\).
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