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A cube has sides of length L = 0.300 m. ...

A cube has sides of length `L = 0.300 m`. It is placed with one corner at the origin ( refer to Fig.2.119).The electric field is not uniform but is given by `vec( E) = ( -5.00 NC^(-1)) x hat(i) + (3.00 NC^(-1)) z hat(k)`.
The total electric charge inside the cube is

A

`- 0.054 epsilon_(0) C`

B

`0.081 epsilon_(0) C`

C

`0.135 epsilon_(0) C`

D

` 0.054 epsilon_(0) C`

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The correct Answer is:
To find the total electric charge inside the cube given the electric field, we can use Gauss's law, which states: \[ \Phi_E = \frac{Q_{enc}}{\epsilon_0} \] where \(\Phi_E\) is the electric flux through a closed surface, \(Q_{enc}\) is the total charge enclosed by the surface, and \(\epsilon_0\) is the permittivity of free space, approximately \(8.85 \times 10^{-12} \, \text{C}^2/\text{N m}^2\). ### Step 1: Calculate the Electric Flux through Each Face of the Cube The electric field is given by: \[ \vec{E} = (-5.00 \, \text{N/C}) \hat{i} + (3.00 \, \text{N/C}) \hat{k} \] The cube has 6 faces, and we need to calculate the electric flux through each face. #### Face 1 (x = 0): - Area vector \(\vec{A_1} = L^2 \hat{i}\) - \(\Phi_1 = \vec{E} \cdot \vec{A_1} = (-5.00) \cdot (0.3^2) = -0.45 \, \text{N m}^2/\text{C}\) #### Face 2 (x = L): - Area vector \(\vec{A_2} = -L^2 \hat{i}\) - \(\Phi_2 = \vec{E} \cdot \vec{A_2} = (-5.00) \cdot (0.3^2) = -0.45 \, \text{N m}^2/\text{C}\) #### Face 3 (y = 0): - Area vector \(\vec{A_3} = L^2 \hat{j}\) - \(\Phi_3 = \vec{E} \cdot \vec{A_3} = 0\) (since \(\hat{j}\) is perpendicular to \(\vec{E}\)) #### Face 4 (y = L): - Area vector \(\vec{A_4} = -L^2 \hat{j}\) - \(\Phi_4 = \vec{E} \cdot \vec{A_4} = 0\) #### Face 5 (z = 0): - Area vector \(\vec{A_5} = L^2 \hat{k}\) - \(\Phi_5 = \vec{E} \cdot \vec{A_5} = (3.00) \cdot (0.3^2) = 0.27 \, \text{N m}^2/\text{C}\) #### Face 6 (z = L): - Area vector \(\vec{A_6} = -L^2 \hat{k}\) - \(\Phi_6 = \vec{E} \cdot \vec{A_6} = (3.00) \cdot (0.3^2) = 0.27 \, \text{N m}^2/\text{C}\) ### Step 2: Sum the Electric Flux Now, we sum the flux through all the faces: \[ \Phi_E = \Phi_1 + \Phi_2 + \Phi_3 + \Phi_4 + \Phi_5 + \Phi_6 \] \[ \Phi_E = (-0.45) + (-0.45) + 0 + 0 + 0.27 + 0.27 = -0.36 \, \text{N m}^2/\text{C} \] ### Step 3: Use Gauss's Law to Find the Charge Using Gauss's law: \[ \Phi_E = \frac{Q_{enc}}{\epsilon_0} \] Rearranging gives: \[ Q_{enc} = \Phi_E \cdot \epsilon_0 \] Substituting the values: \[ Q_{enc} = -0.36 \cdot (8.85 \times 10^{-12}) = -3.19 \times 10^{-12} \, \text{C} \] ### Final Answer The total electric charge inside the cube is approximately: \[ Q_{enc} \approx -3.19 \, \text{pC} \]

To find the total electric charge inside the cube given the electric field, we can use Gauss's law, which states: \[ \Phi_E = \frac{Q_{enc}}{\epsilon_0} \] where \(\Phi_E\) is the electric flux through a closed surface, \(Q_{enc}\) is the total charge enclosed by the surface, and \(\epsilon_0\) is the permittivity of free space, approximately \(8.85 \times 10^{-12} \, \text{C}^2/\text{N m}^2\). ...
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CENGAGE PHYSICS ENGLISH-ELECTRIC FLUX AND GAUSS LAW-Comprehension
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