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.
Step 1: Visualize the Cube and Electric Field
The electric field is in the x-direction and its magnitude varies with x. The cube has side length \(a\).
Step 2: Calculate the Electric Flux
The electric flux through a surface is given by:
\[
\Phi = \int \vec{E} \cdot \vec{A}
\]
Since the electric field is only in the x-direction, the only flux is through the face of the cube at \(x = a\) (the face ABCD in the given figure). The electric field at this face is
\(\vec{E} = E_0a \hat{i}\), and the area vector is \(a^2 \hat{i}\). Therefore, the net flux through the cube is:
\[
\Phi_{\text{net}} = \Phi_{\text{ABCD}} = E_0a \cdot a^2 = E_0a^3
\]
Step 3: Apply Gauss’s Law
Gauss’s law states that the net electric flux through a closed surface is equal to the enclosed charge divided by the permittivity of free space (\(\epsilon_0\)):
\[
\Phi_{\text{net}} = \frac{q_{\text{en}}}{\epsilon_0}
\]
where \(q_{\text{en}}\) is the enclosed charge.
Step 4: Calculate the Enclosed Charge
Combining the flux calculation and Gauss’s law, we have:
\[
\frac{q_{\text{en}}}{\epsilon_0} = E_0a^3
\]
\[
q_{\text{en}} = E_0\epsilon_0a^3
\]
Substitute the given values, \(E_0 = 4 \times 10^4 \, \text{N/Cm}\), \(a = 2 \, \text{cm} = 2 \times 10^{-2} \, \text{m}\), and \(\epsilon_0 = 9 \times 10^{-12} \, \text{C}^2/\text{Nm}^2\):
\[
q_{\text{en}} = (4 \times 10^4) \times (9 \times 10^{-12}) \times (2 \times 10^{-2})^3
\]
\[
q_{\text{en}} = 36 \times 10^{-8} \times 8 \times 10^{-6} = 288 \times 10^{-14} \, \text{C}
\]
Step 5: Find the Value of Q
The enclosed charge is given as \(Q \times 10^{-14} \, \text{C}\). We have found \(q_{\text{en}} = 288 \times 10^{-14} \, \text{C}\). Therefore, \(Q = 288\).
Conclusion: The value of \(Q\) is 288.
The correct answer is 288.
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 \( y = f(x) \) be the solution of the differential equation
\[ \frac{dy}{dx} + 3y \tan^2 x + 3y = \sec^2 x \]
such that \( f(0) = \frac{e^3}{3} + 1 \), then \( f\left( \frac{\pi}{4} \right) \) is equal to:
Find the IUPAC name of the compound.
If \( \lim_{x \to 0} \left( \frac{\tan x}{x} \right)^{\frac{1}{x^2}} = p \), then \( 96 \ln p \) is: 32
It is the property of subatomic particles that experiences a force when put in an electric and magnetic field.
It is a property associated with each point in space when charge is present in any form. The magnitude and direction of the electric field are expressed by E, called electric field strength or electric field intensity.
Electric charges are of two types: Positive and Negative. It is commonly carried by charge carriers protons and electrons.
Various properties of charge include the following :-
Two kinds of electric charges are there :-
When there is an identical number of positive and negative charges, the negative and positive charges would cancel out each other and the object would become neutral.