Problem 11
Question
Go Figure \(23-35\) shows a closed Gaussian surface in the shape of a cube of edge length \(2.00 \mathrm{~m},\) with one corner at \(x_{1}=5.00 \mathrm{~m}\), \(y_{1}=4.00 \mathrm{~m} .\) The cube lies in a region where the electric field vector is given by \(\vec{E}=-3.00 \mathrm{i}-4.00 y^{2} \mathrm{j}+3.00 \mathrm{k} \mathrm{N} / \mathrm{C},\) with \(y\) in meters. What is the net charge contained by the cube?
Step-by-Step Solution
Verified Answer
The net charge contained by the cube is zero.
1Step 1: Calculate Electric Flux through Cube Faces
The electric flux through a closed surface is given by Gauss's law as the sum of electric flux through each face of the cube. The general formula for electric flux through a surface is \( \Phi = \int \vec{E} \cdot d\vec{A} \). For each face of the cube, we need to integrate the dot product of the electric field \( \vec{E} \) and the area vector \( d\vec{A} \).
2Step 2: Evaluate Area Vectors for Cube Faces
For a cube with side length 2 m, the area of each face is \( A = 4 \, \text{m}^2 \). The area vector, \( d\vec{A} \), points perpendicular to the surface: - Front and back faces (xy-plane): \( d\vec{A} = (4 - y^2)\hat{j} \)- Left and right faces (yz-plane): \( -3 \hat{i} \) - Top and bottom faces (xz-plane): \( 3 \hat{k} \)
3Step 3: Calculate Flux through Each Face
- **Left and Right Faces:** Across the left face, where \( x = 5 \), and right face where \( x = 7 \), the electric field is uniform and can be solved by multiplying by area.- **Top and Bottom Faces:** With the bottom face at \( y=4 \) and top at \( y=6 \), since \( E_y = -4y^2 \), perform the integral geometrically across length \(-4\) to \(6 \) for \( y \).- **Front and Back Faces:** Calculate similar to left and right faces similar.Perform these calculations to find the flux through each from the same plane set from the cube dimensions.
4Step 4: Sum Electric Fluxes to Find Net Flux
Sum the electric flux values from all six faces of the cube. By Gauss's law, the sum of the fluxes will give the total flux through the surface: \(\Phi_{net} = \Phi_{front} + \Phi_{back} + \Phi_{left} + \Phi_{right} + \Phi_{top} + \Phi_{bottom}\)
5Step 5: Apply Gauss's Law to Find Net Charge
According to Gauss's Law, the net electric flux through a closed surface is related to the net charge \( Q_{enc} \) enclosed by the surface by \( \Phi_{net} = \frac{Q_{enc}}{\varepsilon_0} \). Rearrange to find the net charge: \( Q_{enc} = \Phi_{net} \cdot \varepsilon_0 \), where \( \varepsilon_0 = 8.85 \times 10^{-12} \, \text{C}^2/\text{N} \, \text{m}^2 \).
Key Concepts
Electric FluxClosed SurfaceNet ChargeGaussian Surface
Electric Flux
Electric flux is a measure of the electric field passing through a certain area. Imagine it like wind passing through a net. The amount of air (wind) that goes through depends on both the strength of the wind and the size of the net. Similarly, electric flux depends on the strength of the electric field and the angle at which the field lines pass through the surface.
The mathematical expression for electric flux, \( \Phi \), through a surface area \( A \) is given by:
The mathematical expression for electric flux, \( \Phi \), through a surface area \( A \) is given by:
- \( \Phi = \int \vec{E} \cdot d\vec{A} \)
Closed Surface
A closed surface is a boundary that encases a volume entirely, like a bubble wrapping around a bunch of soap. In physics, especially electromagnetism, closed surfaces are vital because they allow us to apply Gauss's Law. A cube, as presented in the exercise, serves as a perfect example of a closed surface.
Each face of the cube contributes separately to the total electric flux due to its orientation. For a closed surface, such as this cube, every face needs evaluation. This approach ensures that all the electric field lines entering or exiting the enclosed space are accounted for. The closed surface aids us in determining the net charge inside the volume through Gauss's Law.
Each face of the cube contributes separately to the total electric flux due to its orientation. For a closed surface, such as this cube, every face needs evaluation. This approach ensures that all the electric field lines entering or exiting the enclosed space are accounted for. The closed surface aids us in determining the net charge inside the volume through Gauss's Law.
Net Charge
The net charge refers to the total charge contained within a closed surface. This is an essential value to determine because it gives insight into the electric state within that surface. Thanks to Gauss's Law, we have a powerful way to connect electric flux and the net charge.
According to Gauss's Law, the net electric flux through a closed surface equals the net charge inside, divided by the permittivity of free space, \( \varepsilon_0 \):
According to Gauss's Law, the net electric flux through a closed surface equals the net charge inside, divided by the permittivity of free space, \( \varepsilon_0 \):
- \( \Phi_{net} = \frac{Q_{enc}}{\varepsilon_0} \)
- Rearranging gives: \( Q_{enc} = \Phi_{net} \cdot \varepsilon_0 \)
Gaussian Surface
A Gaussian surface is a theoretical concept used in Gauss's Law to simplify the calculation of electric flux and the net charge enclosed. This entirely imaginary surface helps by enclosing charges symmetrically, allowing easy computation of the electric field's effect.
The choice of Gaussian surface depends on the symmetry of the problem. Common Gaussian shapes include spheres, cylinders, and cubes - like the cube in the exercise. The beauty of using a Gaussian surface lies in its ability to simplify complex electromagnetism problems through easier calculations of flux.
The choice of Gaussian surface depends on the symmetry of the problem. Common Gaussian shapes include spheres, cylinders, and cubes - like the cube in the exercise. The beauty of using a Gaussian surface lies in its ability to simplify complex electromagnetism problems through easier calculations of flux.
- For example, in a cube, each face becomes a convenient plane to assess the contribution of the electric field.
- The symmetry of the surface and field determines how simply we can apply Gauss's Law.
Other exercises in this chapter
Problem 9
Fig. 23-31 shows a Gaussian surface in the shape of a cube with edge length \(1.40 \mathrm{~m}\). What are (a) the net flux \(\Phi\) through the surface and (b)
View solution Problem 10
Figure 23-34 shows a closed Gaussian surface in the shape of a cube of edge length \(2.00 \mathrm{~m} .\) It lies in a region where the nonuniform electric fiel
View solution Problem 13
The electric field in a certain region of Earth's atmosphere is directed vertically down. At an altitude of \(300 \mathrm{~m}\) the field has magnitude \(60.0 \
View solution Problem 15
A particle of charge \(+q\) is placed at one corner of a Gaussian cube. What multiple of \(q / \varepsilon_{0}\) gives the flux through (a) each cube face formi
View solution