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Using Gauss's law and assuming the pipe is sufficiently long to consider it infinitely long, calculate...

Using Gauss's law and assuming the pipe is sufficiently long to consider it infinitely long, calculate the electric field r = 6.51 cm from the centerline of the pipe.

Using Gauss's law and assuming the pipe is suffici

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Answer #1

Draw a "hypothetical" pipe of radius r=0.0651m (same radius you want to know the field) and concentric with the actual pipe. Let it have arbitrarly length "L".
From symmetry you assume the E-field is along "r" , hence perpendicular to your hypothetical pipe and also constant on the surface "A" of that pipe, since r is constant.
You then evaluate the left side of Gauss Law. Because E is constant on the surface and crosses the curved portion perpendicularly (its parallel to the area vector) the integral is just "EA" . There is no contribution from the caps of the pipe because E does not penetrate the caps, just slides over them.
So now Gauss' law reduces to; eoEA = Q

Where A = 2pi*r*L
and where "Q" is the net charge enclosed by your hypothetical pipe.
Since it encloses a section of actual pipe ,of length L, you find Q by multiplying the charge density "D" times the volume of the pipe thickness;
Q = D[pi*Ro^2*L - pi*Ri^2*L] , Where Ro & Ri are the outer and inner radii of the pipe, in meters.

So the E-field is then; after cancelling "L" and "pi";
E = (D/2eor)[Ro^2 - Ri^2] = [(0.00122)/(2*8.85*10^-12*0.0651)]*[0.0310^2 - 0.0264^2]

E = 279560.17 N/C

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