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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 asE.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

Question: If the electric field in some region is given (in spherical coordinates)

by the expression

E(r)=kr[3r^+2sinθcosθsinϕθ^+sinθcosϕϕ^]

for some constant , what is the charge density?

(a) Check that the results of Exs. 2.5 and 2.6, and Prob. 2.11, are consistent with Eq. 2.33.

(b) Use Gauss's law to find the field inside and outside a long hollow cylindrical

tube, which carries a uniform surface charge σ.Check that your result is consistent with Eq. 2.33.

(c) Check that the result of Ex. 2.8 is consistent with boundary conditions 2.34 and 2.36.

Findthe electric field a distance zfrom the center of a spherical surface of radius R(Fig. 2.11) that carries a uniform charge density σ.Treat the case z< R(inside) as well as z> R(outside). Express your answers in terms of the total chargeqon the sphere. [Hint:Use the law of cosines to write rin terms of Rand θ.Besure to take the positivesquare root:R2+z2-2Rz=(R-z)if R>z,but it's(z-R)if R<z.]

In a vacuum diode, electrons are "boiled" off a hot cathode, at potential zero, and accelerated across a gap to the anode, which is held at positive potential V0. The cloud of moving electrons within the gap (called space charge) quickly builds up to the point where it reduces the field at the surface of the cathode to zero. From then on, a steady current I flows between the plates.

Suppose the plates are large relative to the separation (A>>d2in Fig. 2.55), so

that edge effects can be neglected. Then V,ρand v (the speed of the electrons) are all functions of x alone.

  1. Write Poisson's equation for the region between the plates.

  1. Assuming the electrons start from rest at the cathode, what is their speed at point x , where the potential is V(x)?

  1. In the steady state, I is independent of x. What, then, is the relation between p and v?

  1. Use these three results to obtain a differential equation for V, by eliminating ρand v.

  1. Solve this equation for Vas a function of x, V0and d. Plot V(x), and compare it to the potential without space-charge. Also, find ρand v as functions of x.

  1. Show that
    I=kV03/2

and find the constant K. (Equation 2.56 is called the Child-Langmuir law. It holds for other geometries as well, whenever space-charge limits the current. Notice that the space-charge limited diode is nonlinear-it does not obey Ohm's law.)

Find the electric field a distance zabove the center of a circular loop of radius r(Fig. 2.9) that carries a uniform line charge λ

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