CSS-1 Two very long thin concentric shells have charge evenly distributed over their surfaces. The inner shell of radius ₁-R has suface charge density +o. The outer shell of radius 12-2R has suface charge density -20 (twice the magnitude and of opposite sign to the inner shell). Side view: to .c .b .d 0 -Z End view: R .C .b -20 '2R c) You are going to apply Gauss' law to find the magnitude of the electric field at point 'b'. Draw on both views of your figure an appropriate Gaussian surface that can be used to find Ep. Show on your figures representative area vector elements, dA for each distinct part of your gaussian surface (that passes thru point 'b'). Apply Gauss' law EdA=qend/s, to find an expression for the electric field at 'b' in terms of o and any other constants (but not in terms of q). d) Repeat step c) to find the electric field strength at point 'c'. You may modify your results from b) as appropriate. e) Repeat step c) to find the electric field strength at point 'd'. You may modify your results from b) as appropriate. Point d is within the cavity inside of the inner shell.

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CSS-1 Two very long thin concentric shells have charge evenly distributed over their surfaces. The inner shell
of radius 1₁-R has suface charge density +o. The outer shell of radius r2-2R has suface charge density
-20 (twice the magnitude and of opposite sign to the inner shell).
Side view:
to
A
.c
.b
.d
0
Z
End view:
R
.C
.b
.d
-20
*2R
c) You are going to apply Gauss' law to find the magnitude of the electric field at point 'b'. Draw on both
views of your figure an appropriate Gaussian surface that can be used to find Eb. Show on your figures
representative area vector elements, dA for each distinct part of your gaussian surface (that passes thru
point 'b'). Apply Gauss' law EdA=qend/Eo to find an expression for the electric field at 'b' in terms of
o and any other constants (but not in terms of q).
d) Repeat step c) to find the electric field strength at point 'c'. You may modify your results from
b) as appropriate.
e) Repeat step c) to find the electric field strength at point 'd'. You may modify your results from
b) as appropriate. Point d is within the cavity inside of the inner shell.
Transcribed Image Text:CSS-1 Two very long thin concentric shells have charge evenly distributed over their surfaces. The inner shell of radius 1₁-R has suface charge density +o. The outer shell of radius r2-2R has suface charge density -20 (twice the magnitude and of opposite sign to the inner shell). Side view: to A .c .b .d 0 Z End view: R .C .b .d -20 *2R c) You are going to apply Gauss' law to find the magnitude of the electric field at point 'b'. Draw on both views of your figure an appropriate Gaussian surface that can be used to find Eb. Show on your figures representative area vector elements, dA for each distinct part of your gaussian surface (that passes thru point 'b'). Apply Gauss' law EdA=qend/Eo to find an expression for the electric field at 'b' in terms of o and any other constants (but not in terms of q). d) Repeat step c) to find the electric field strength at point 'c'. You may modify your results from b) as appropriate. e) Repeat step c) to find the electric field strength at point 'd'. You may modify your results from b) as appropriate. Point d is within the cavity inside of the inner shell.
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