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A Gaussian surface in the form of a hemisphere of radiusR=5.68cmlies in a uniform electric field of magnitudeE=2.50 N/C. The surface encloses no net charge. At the (flat) base of the surface, the field is perpendicular to the surface and directed into the surface. What is the flux through

(a) the base and

(b) the curved portion of the surface?

Short Answer

Expert verified

a) The flux through the base of the surface is -0.0253 N⋅m2/C.

b) The flux through the curved portion of the surface is 0.0253 N⋅m2/C.

Step by step solution

01

The given data

a) The gaussian hemispherical surface of the radius,R=5.68 cm.

b) The magnitude of the electric field,E=2.50N/C.

02

Understanding the concept of the electric flux

Using the concept of the Gauss flux theorem, we can get the required value of the flux passing through the base area of the surface. Now, using the concept of the net charge to be zero for a Gaussian surface, we can get the electric flux through the curved surface.

Formula:

The electric flux passing through any surface, ϕ=E→.A→ (i)

03

a) Calculation of the flux through the base area of the surface

We choose a coordinate system whose origin is at the center of the flat base, such that the base is in the x-y plane and the rest of the hemisphere is in thez>0 half-space.

Now, using the given data and area of the circular base,A=Ï€¸é2 in equation (i), we can get the electric flux through the base surface as given:

Ï•=Ï€¸é2-k^.Ek^=-Ï€¸é2E=-Ï€0.0568m22.50N/C=-0.0253 Nâ‹…m2/C

Hence, the value of the flux is -0.0253 N⋅m2/C.

04

b) Calculation of the flux through the curved area of the surface

Since the flux through the entire hemisphere is zero, the flux through the curved surface is given as:

ϕC=ϕbase=0.0253Nm2/C

Hence, the value of the flux is 0.0253Nm2/C.

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Most popular questions from this chapter

A non-conducting solid sphere has a uniform volume charge density P. Letr→be the vector from the center of the sphere to a general point Pwithin the sphere.

(a) Show that the electric field at Pis given byE⃗=Òϰù⃗/3ε0(Note that the result is independent of the radius of the sphere.)

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