A 1.0cm×1.0cm×1.0cm box with its edges aligned with the xyz-axes is in the electric field E=(350x+150)i^N/C, where x is in meters. What is the net electric flux through the box?

Short Answer

Expert verified

The net electric flux through the box isΦ=3.5×10-4Nm/C

Step by step solution

01

Given information and Theory used 

Given :

Dimensions of the box : 1.0cm×1.0cm×1.0cm

The electric field is : E=(350x+150)i^N/C

Theory used :

The net electric flux through the surface of a box is directly proportional to the magnitude of the net charge enclosed by the box. The net electric flux due to a point charge inside a box is independent of box's size, only depends on net amount of charge enclosed.

02

Calculating the net electric flux through the box 

The field points along the x-axis so it is parallel to all the four faces that encircle it and it's perpendicular to the two faces as in the figure bellow.

Therefore, all of the four faces that are parallel to the field don't contribute to net flux, only the two faces perpendicular to it do. One of them is x=0so :

E=150iN/C

The other one is x=1.0cm=0.01m, so there are two possibilities.

We get :

E=(350·0.01+150)iN/C=153iN/C

by plugging in the specified numerical numbers.

Now, E1points inside, so the face atx=0contributes negatively, while E2points outside, so the face at x=1.0cmcontributes positively.

So, we have

role="math" localid="1649665790231" Φ=-E1(0.01m)²+E2(0.01m)²=(0.01m)²(E-E).Φ=3.5×10-4Nm/C

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Most popular questions from this chapter

Newton’s law of gravity and Coulomb’s law are both inversesquare laws. Consequently, there should be a “Gauss’s law for gravity.” a. The electric field was defined as E u = F u on q /q, and we used this to find the electric field of a point charge. Using analogous reasoning, what is the gravitational field g u of a point mass?

Write your answer using the unit vector nr, but be careful with signs; the gravitational force between two “like masses” is attractive, not repulsive. b. What is Gauss’s law for gravity, the gravitational equivalent of Equation 24.18? Use ΦG for the gravitational flux, g u for the gravitational field, and Min for the enclosed mass. c. A spherical planet is discovered with mass M, radius R, and a mass density that varies with radius as r = r011 - r/2R2, where r0 is the density at the center. Determine r0 in terms of M and R. Hint: Divide the planet into infinitesimal shells of thickness dr, then sum (i.e., integrate) their masses. d. Find an expression for the gravitational field strength inside the planet at distance r 6 R.

A neutral conductor contains a hollow cavity in which there is a+100nCpoint charge. A charged rod then transfers-50nC to the conductor. Afterward, what is the charge (a) on the inner wall of the cavity, and (b) on the exterior surface of the conductor?

All examples of Gauss's law have used highly symmetric surfaces where the flux integral is either zero or EA. Yet we've claimed that the net Φe=Qin/ϵ0is independent of the surface. This is worth checking. FIGURE CP24.57 shows a cube of edge length Lcentered on a long thin wire with linear charge density λ. The flux through one face of the cube is not simply EA because, in this case, the electric field varies in both strength and direction. But you can calculate the flux by actually doing the flux integral.

a. Consider the face parallel to the yz-plane. Define area dAas a strip of width dyand height Lwith the vector pointing in the x-direction. One such strip is located at position localid="1648838849592" y. Use the known electric field of a wire to calculate the electric flux localid="1648838912266" dΦthrough this little area. Your expression should be written in terms of y, which is a variable, and various constants. It should not explicitly contain any angles.

b. Now integrate dΦto find the total flux through this face.

c. Finally, show that the net flux through the cube is Φe=Qin/ϵ0.

A positive point chargeq sits at the center of a hollow spherical shell. The shell, with radius R and negligible thickness, has net charge -2q. Find an expression for the electric field strength (a) inside the sphere, r<K, and (b) outside the sphere, r>K. In what direction does the electric field point in each case?

FIGUREEX24.18shows three charges. Draw these charges on your paper four times. Then draw two-dimensional cross sections of three-dimensional closed surfaces through which the electric flux is (a) -q/ϵ0, (b) q/ϵ0, (c) 3q/ϵ0, and (d) 4q/ϵ0.

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