PHY2049 - Fall 2016 - HW6 Solutions
PHY2049 - Fall 2016 - HW6 Solutions
Allen Majewski
Department Of Physics, University of Florida
2001 Museum Rd. Gainesville, FL 32611
October 11, 2016
These are solutions to Halliday, Resnick, Walker Chapter 28, No: 10, 16,
30, 35, 38, 39, 51, 65
1
28.10
A proton travels through uniform magnetic and electric fields. The
~ = (?2.50 mT ) i?. At one instant the velocity of
magnetic field is B
the proton is v = (2000 m/s ) j?. At that instant and in unit-vector
notation, what is the net force acting on the proton if the electric
field is (a) (4.00V/m) k? (b) (?4.00 V/m ) k?, and (c) (4.00V/m) i? ?
The Lorentz force invloving both fields is
~
~
~
F = q E + ~v ¡Á B
The proton charge is just e. In all cases ~v = 2000 m/s j? = vy j? and
~
~ = 4.00 k? = Ez k?
B = -2.50 mT i? = Bx i?. For case (a) the electric field is E
?? ? ? ? ? ??
0
0
Bx
~
?
?
?
?
?
?
0 + vy ¡Á 0 ??
F =e
Ez
0
0
You should evaluate the cross product first
1
? ? ? ?
?
?
0
Bx
0
?vy ? ¡Á ? 0 ? = vy Bx (y? ¡Á x?) = vy Bx (?z?) = ? 0 ?
0
0
?vy Bx
Pluggign this into the equations for the Lorentz force we find
?? ? ?
??
0
0
F~ = e ?? 0 ? + ? 0 ??
Ez
?vy Bx
F~ = e (Ez ? vy Bx ) z?
F~ = 1.602x10?19 C 4 V/m ? 2000 m/s -2.5x10?3 T = 1.44x10?18 N k?
~
For (b) and (c), simply evalue this expression for different values of E.
~ is in the x-direction (not z) so you¡¯ll end up with an
Note that in part (c) E
x-component as well as a z-component of the resulting force.
2
28.16
Figure 28-34 shows a metallic block, with its faces parallel to coordinate axes. The block is in a uniform magnetic field of magnitude
0.020 T. One edge length of the block is 25 cm; the block is not
drawn to scale. The block is moved at 3.0 m/s parallel to each
axis, in turn, and the resulting potential difference V that appears
across the block is measured. With the motion parallel to the yaxis, V = 12 mV; with the motion parallel to the z axis, V = 18
mV; with the motion parallel to the x axis, V = 0.What are the
block lengths (a) dx , (b) dy , and (c) dz ?
We make use of the Hall Effect, in which we require that the strength of
force due to the electric field is equal to that of the magnetic field
~ = e ~v ¡Á B
~
eE
|E| = |v| |B|
The hall potential difference is
2
Figure 1: Problem 28.16
V = Ed
Replace E with vB and find
V = vBd
V
=d
vB
0.012 V
= 0.02m
(3.0 m/s) (0.02 T )
0.018 V
dy =
= 0.03m
(3.0 m/s) (0.02 T )
dz =
3
Then dx must be 0.025 m by process of elimination.
3
28.30
Figure 2: Problem 30
In Fig. 28-39, an electron with an initial kinetic energy of 4.0
keV enters region 1 at time t = 0. That region contains a uniform
magnetic field directed into the page, with magnitude 0.010 T.
The electron goes through a half-circle and then exits region 1,
headed toward region 2 across a gap of 25.0 cm. There is an electric
potential difference ?V = 2000 V across the gap, with a polarity
such that the electrons speed increases uniformly as it traverses
the gap. Region 2 contains a uniform magnetic field directed out
of the page, with magnitude 0.020 T. The electron goes through a
half-circle and then leaves region 2. At what time t does it leave?
4
If the electron spends an amount of time t1 in region 1, tgap in the gap,
and t2 in region two, the total time of this journey is
ttotal = t1 + tgap + t2
In regions 1 and 2, the electron makes a half circle
¦ÐR
d
=
v
v
In circular motion due to a magnetic field, we have
t=
v2
= qvB
R
so v = qBR/m and the t becomes
m
t=
¦ÐR
¦Ðm
d
=
=
v
qBR/m
qB
We can use this to get t1 and t2 :
t1 =
¦Ðme
¦Ð 9.109e-31 kg
=
= 1.786 ns
eB1
1.602e-19 C ¡Á 0.01 T
¦Ðme
¦Ð 9.109e-31 kg
=
= 0.893 ns
eB2
1.602e-19 C ¡Á 0.02 T
The time in the gap requires us to do a little work. The electron accelerates trough a potential difference of 2 kV. So it gaines 2 keV of energy. It
enters the gap with Ei = 4 keV and thus leaves with Ef = 6 keV. It is useful
here to know 1 keV = 1.602e-16 J. We express speed in terms of E using
v = 21 mv 2 and find
r
2Ei
vi =
= 3.7509e7 m/s
me
r
2Ef
vf =
= 4.5939e7 m/s
me
We can use the kinematic equation
t2 =
1
(vf + vi ) tgap = d
2
5
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