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A charge q sits at the back comer of a cube, as shown in Fig. 2.17.What is the flux of E through the shaded side?

Short Answer

Expert verified

The electric flux through the shade area is∅=q24ξ0.

Step by step solution

01

Describe the given information

It is given that a charge qsits at the back comer of a cube.as shown in following figure

The flux of electric field through the shaded side need to be evaluated.

02

Define the Gauss law

If there is a surface area enclosing a volume, possessing a charge inside the volume then the electric field due to the surface or volume charge is given as∮E.da=qε0

Hereqis the total charge inside the volume,ε0is the permittivity of free surface.

03

Obtain the electric flux

The left side expression of the gauss law,∮E.da=qencosedE0, that is ∮E.dais called the electric flux and it is equal to the quantity qenclosedε0

There are 4 cubes above the charge 2 cubes at the side of the charge, and 2 cubes below the charge. Thus there are 8 cubes in total surrounding the charge

The charge passes through each cube equally. So, the charge per face of each cube becomes 16.The 16thpart is quarter of the large cube as shown in following figure,

So, the total flux per face of each cube becomes 1614.that is 124.Thus, the flux through the shaded area is

Thus, the electric flux through the shade area is ∅=q24ε0.

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Most popular questions from this chapter

Use your result in Prob. 2.7 to find the field inside and outside a solidsphere of radius Rthat carries a uniform volume charge densityp.Express your answers in terms of the total charge of the sphere,q.Draw a graph of lEIas a function of the distance from the center.

Suppose the plates of a parallel-plate capacitor move closer together by an infinitesimal distance∈, as a result of their mutual attraction.

(a) Use Eq. 2.52 to express the work done by electrostatic forces, in terms of the fieldE, and the area of the plates, A.

(b) Use Eq. 2.46 to express the energy lost by the field in this process.

(This problem is supposed to be easy, but it contains the embryo of an alternative derivation of Eq. 2.52, using conservation of energy.)

We know that the charge on a conductor goes to the surface, but just

how it distributes itself there is not easy to determine. One famous example in which the surface charge density can be calculated explicitly is the ellipsoid:

x2a2+y2b2+z2c2=1

In this case15

σ=Q4πabc(x2a4+y2b4+z2c4)-1/2

(2.57) where Q is the total charge. By choosing appropriate values for a , b and c. obtain (from Eq. 2.57):

(a) the net (both sides) surface charge density a(r) on a circular disk of radius R; (b) the net surface charge density a(x) on an infinite conducting "ribbon" in the xy plane, which straddles they axis from x = - a to x = a (let A be the total charge per unit length of ribbon);

(c) the net charge per unit length λ(x)on a conducting "needle," running from x = - a to x = a. In each case, sketch the graph of your result.

Two infinitely long wires running parallel to the x axis carry uniform

charge densities +λand-λ.

(a) Find the potential at any point(x,y,z)using the origin as your reference.

(b) Show that the equipotential surfaces are circular cylinders, and locate the axis

and radius of the cylinder corresponding to a given potential .

(a) A point chargeqis inside a cavity in an uncharged conductor (Fig. 2.45). Is the force onq necessarily zero?

(b) Is the force between a point charge and a nearby uncharged conductor always

attractive?

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