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wangsness electromagnetic fields solutions - HW - Ch4ch5, Notas de estudo de Física

wangsness electromagnetic fields solutions

Tipologia: Notas de estudo

2017

Compartilhado em 22/01/2017

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Homework 2
4-2.A sphere
of
radius a
has
its center at the origin and a charge density given
by
p =Ar2 A =
constant. Another
of
radius
is
concentric
with
the first.
Find
the flux
cj
E.
dii
through the
surface
of
the larger sphere.
From Gauss'
Law,
Because spheres are concentric,
The total
Qin
of
smaller
can
be
by
21r
1r
Qin
= 1
p(r')
dr'
r r
fa
p(r')(r')2
sin
B'
dr'
dB' dq/
V(a)
)0 )0
0
(1r
r
1r
fa
A(r')2(r')2 dr'
dB'
dq/
A
f21r
J1r
~
sin
B'
dB'
dq/
)0
Jo 0 0 0 5
EO
contains
21r
2Aa5
5
1+1
5
J
o
hl'>r,,,,tnlrl'> the flux through surface
of
larger
5
Qin
is
=--
1
pf3
pf4

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Homework 2

4-2.A sphere of radius a has its center at the origin and a charge density given by p = Ar2 A =

constant. Another of radius is concentric with the first. Find the flux cj E. dii through the

surface of the larger sphere. From Gauss' Law,

Because spheres are concentric, The total Qin of smaller can be by 21r (^) 1r Qin = 1 p(r') dr' r r fa p(r')(r')2 sin B' dr' dB' dq/ V(a) )0 )0 0 (1r r

1r

fa A(r')2(r')2 dr' dB' dq/ A f21r J1r ~ (^) sin B' dB' dq/

)0 Jo 0 0 0 5

EO

contains

21r 2Aa

(^5) J 1+1 5 o hl'>r,,,,tnlrl'> the flux through (^) surface of larger

Qin

is

by an infinitely long cylinder of axis coincides with the line of the cylinder carries a of constant density cr. Find E everywhere. What particular value of cr will make E = 0 for all the charged cylinder? Is your answer

Due to both the cylinder and line length,^ E cannot depend on^ our^ I",..':of-ir....^ on^ z-axis

Due to symmetry of the line & E cannot on our <p in

must be (^) P component. E = Ep(P)fi.

  • Case 1 : P < Po The cylinder around the line charge behaves similar to a conductor where the charge lies on the surface.

Inside any conductor, the electric field from surface charge is zero, thus ECYlinder = 0 in this case.

Thus, this case simply becomes the scenario a line charge where

A " (4 - 11)

2rcEopP,

  • Case 2 : Po < P

= f/p(p)p, ftc +

Qin

L

Ep (P)2rcpL

If E = 0 when Po < P, then

A+

Which makes sense, as 2rcPo(J -A, providing equal and opposite to the line

for any desired length.

.. What is the smallest value of z which the potential due to the disc can be calculated as if it were a point without an error greater than 1 percent? For a point potential is calculated by 4>(T) = Q, (S The charge Q the circular disc is calculated by Q = rra^2 q Thus, treating the disc as a pOint charge z axis, potential is calculated by rra^2 q

4>(z) = =

In to have accuracy desired,

-0.01 <

a^2 q

< 0.01 => -0.01 < 1 - q^ 41zlEo < 0.

2100 [(a^

(^2) + Z2)1/2 -Izl]

0.99 < 2 [( az 2 2 + < 1.01 => < -z 2 <

a^2 a^2 a^2 2.02 <^ +^ Z^ 4)1/2^ _^ <^ 1.98 ->..-I'^ 2.02 +^ < (^ a^2 z 2 +^ <^ 1.98+ a^4 a^2 z^2 a^2 z 2 4.0804 + 1.01 + Z4 < + Z4 < 3.9204 + 0.99 +

4.0804 -101 < 0 <--+ 99 a^2 101 > 4.0804 => Izi >^ --a;:::::^ ..J25a^ =^ Sa

Therefore, in order to calculate the potential as a point charge without an error^ than 1^ no,',..o.,1"

z must be than;::::: Sa.