A point charge of magnitude q is at the center of a cube with sides of length L.a) What is the electric flux through each of the six faces of the cube?b) What would be the flux through a face of the cube if its sides were of length L1?

Respuesta :

The flux through each face is q/6ε₀ .

Explanation:

The charge q is placed at the center of the cube of side L

According to Gauss's law the flux through any closed surface is q/ε₀

here q is the charge enclosed .

In this case cube has the six faces . The flux through each face = q/6ε₀

In the second case The cube has the face with length L₁

The flux through each face = q/6ε₀

Thus flux through the cube does not depend upon the size of the cube .

a) The electric flux through the six faces of the cube is [tex]\phi_{E} = \frac{q}{\epsilon_{o}}[/tex].

b) The electric flux through a face of the cube is [tex]\phi_{E'} = \frac{q}{6\cdot \epsilon_{o}}[/tex].

By the Gauss's Law, the net electric flux of a given close surface is equal to the electric charge within divided by electric permitivity. The definition of the Gauss's Law is described below:

[tex]\phi_{E} = \oint_{S}\,\vec E\,\bullet\,d\vec A = \frac{q}{e_{o}}[/tex] (1)

Where:

[tex]\phi_{E}[/tex] - Electric flux, in newton-square meters per coulomb.

[tex]\vec E[/tex] - Electric field, in newtons per coulomb.

[tex]d \vec A[/tex] - Infinitesimal vector area, in square meters.

[tex]q[/tex] - Electric charge enclosed in the cube, in coulombs.

[tex]\epsilon_{o}[/tex] - Electric permitivity, in farads per meter.

As we know that point charge is centered and cube has six faces with same surface area and same configuration, we can expand (1) by principle of symmetry:

[tex]\phi_{E} = 6\cdot \oint_{S} \vec E \,\bullet \,d\vec A = \frac{q}{\epsilon_{o}}[/tex] (2)

a) The electric flux through the six faces of the cube is [tex]\phi_{E} = \frac{q}{\epsilon_{o}}[/tex].

b) The electric flux through a face of the cube is [tex]\phi_{E'} = \frac{q}{6\cdot \epsilon_{o}}[/tex].

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