Download - COULOMB ’ S LAW, E FIELDS
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COULOMB’S LAW, E FIELDS
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Class ActivitiesCoulomb’s Law
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Class Activities: Charge Distibutions
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Two charges +Q and -Q are fixed a distance r apart. The direction of the force on a test charge -q at A is…
A.UpB.DownC.LeftD.RightE.Some other direction,
or F =0
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Two charges +q and -q are on the y-axis, symmetric about the origin. Point A is an empty point in space on the x-axis. The direction of the E field at A is…A.UpB.DownC.LeftD.RightE.Some other direction, or E = 0, or ambiguous
2.3
+q
x
y
-q
A
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How is the vector related to r1 and r2?
r2
r1
2.1b
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Coulomb's law:
In the fig, q1 and q2 are 2 m apart. Which arrow can represent ?
q1 q2
A
B C
D) More than one (or NONE) of the aboveE) You can't decide until you know if q1 and q2 are the same or opposite signed charges
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What is ("from 1 to the point r") here?
+qr1=(x1,y1) -q
r=(x,y)
2.2
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Only click when you are DONE with page 1 (Part 1 i-iii)
Is the answer to part 1- iiiA) A sum?B) An integral over dy?C) An integral over something else?
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Tutorial 1, part 2- Script rOnly after you finish Part 2, what is in part 2-iv ?
E) None of these!
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5 charges, q, are arranged in a regular pentagon, as shown. What is the E field at the center?
A) ZeroB) Non-zeroC) Really need trig and a calculator to
decide
q
q
q
2.5
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1 of the 5 charges has been removed, as shown. What’s the E field at the center?
q
q
A) +(kq/a2) jB) -(kq/a2) jC) 0D) Something entirely different!E) This is a nasty problem which I need more
time to solve
+x
+ya
2.6
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To find the E- field at P=(x,y,z) from a thin line (uniform linear charge density ):
What is ?
A) X B) y'
C) D)
E) Something completely different!!
P=(x,0,0)x
y
dl'r'
r
2.10
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P=(x,0,0)x
y
dl'r'=(0,y',0)
r
2.11
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,so
P=(x,0,0)x
y
dl'r'=(0,y',0)
r
2.11
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To find the E- field at P from a thin ring (radius R, uniform linear charge density ):
what is ?
P=(0,0,z)
R xy dl'
B
E) NONE of the arrows shown correctly represents
A CD
2.12
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To find the E- field at P from a thin ring (radius a, uniform linear charge density ):
what is ?A)
B) a
C) D) z
E) Something completely different!!
P=(0,0,z)
a x
y dl'
2.13
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Griffiths p. 63 finds E a distance z from a line segment with charge density :
What is the approx. form for E, if z>>L?
A) 0 B) 1 C) 1/z D) 1/z^2 E) None of these is remotely correct.
x
(0,0,z)
-L +L
2.16
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Griffiths p. 63 finds E a distance z from a line segment with charge density :
What is the approx. form for E, if z<<L?
A) 0 B) 1 C) 1/z D) 1/z^2 E) None of these is remotely correct.
x
(0,0,z)
-L +L
2.16
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D) None of these
To find E at P from a negatively charged sphere (radius R, uniform volume charge density ) using
what is (given the small volume element shown)? P=(x,y,z)
x
yz(x’,y’,z’)
R A
BC
2.14
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A)
B)
C)
D) E) None of these
P=(X,Y,Z)
X,Y,Z
(X x)2
(Y y)2
(Z z)2
dxdydz
X,Y,Z (X x)2 (Y y)2 (Z z)2 3/2
dxdydz
X x,Y y,Z z
(X x)2
(Y y)2
(Z z)2
dxdydz
X x,Y y,Z z (X x)2 (Y y)2 (Z z)2 3/2
dxdydz
140
(....?)
x
yz(x,y,z)
R
2.15
dq
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A)
B)
C)
D) E) None of these
P=(X,Y,Z)
X,Y,Z
(X x)2
(Y y)2
(Z z)2
dxdydz
X,Y,Z (X x)2 (Y y)2 (Z z)2 3/2
dxdydz
X x,Y y,Z z
(X x)2
(Y y)2
(Z z)2
dxdydz
X x,Y y,Z z (X x)2 (Y y)2 (Z z)2 3/2
dxdydz
140
(....?)
x
yz(x,y,z)
R
2.15