Title: phy202_7
1Lesson 7
Magnetic Fields
- Magnetic Force on moving charge
- Motion of charge in Magnetic Field
- Magnetic Force on current carrying conductor
- Torque on current carrying loop
- Hall Effect
- Magnetic Devices
2Magnetic Force
- Some metallic objects cause other metallic
objects to accelerate - Thus must be producing a force
- This force is different to Gravitational Force
and Electric Force - Can plot the directions of lines field
- By alignment of magnetic dipoles
- MAGNETIC FORCE
3Magnetic Field Lines
4Properties of Magnetic Fields
- Properties
- Moving charge (current) is effected
- Force proportional
- Q and v
- FB 0 if v parallel to Magnetic Field B
- FB perpendicular to v and B
- FB on positive charge opposite to that on
negative charge - FB proportional to Sin of the angle v makes
with B
5Mathematical Expression
6Vector Product I
Vector Product
A
i
j
k
A
A
A
x
y
z
B
i
j
k
B
B
B
x
y
z
i
j
k
A
A
A
A
A
A
y
z
x
y
x
z
-
A
B
i
j
k
A
A
A
x
y
z
B
B
B
B
B
B
y
z
x
y
x
z
B
B
B
x
y
z
(
)
(
)
(
)
-
-
-
-
i
j
k
A
B
A
B
A
B
A
B
A
B
A
B
y
z
z
y
x
z
z
x
x
y
y
x
7Vector Product II
8Unit vector products
9Work done by Magnetic Field
Work Done by Magnetic Force on charge
10Work done by Electric Field
Compare to Electric Force
11Implications
- Thus Kinetic Energy of charge is not changed by
FB - Potential Energy is not changed
1
1
-
2
2
DK
m
m
vf
0
vi
2
2
Þ
vi
vf
B
i
.
e
.
speed is constant under influence of
v
but
can change direction
12SI units
13Magnetic Flux
Magnetic Flux
F
B
For constant magnetic field over flat area
B
with area vector
A
F
B
AABcosq
B
in general
ò
F
B
A
d
B
surface
F
2
Tm
Wb
(
Weber
)
B
14Right Hand Rule for Magnetic Force
15Magnetic Force on Moving Charge
FB
B
v
Q
k
j
i
-
F
v
B
Q
j
k
Q
v
B
B
y
z
i
j
k
-
-
-
j
k
i
Qv
B
Qv
B
0
1
0
Qv
B
y
z
y
z
y
z
0
0
1
16Mathematical expression
17Uniform Circular Motion of Charge
Uniform Circular Motion
18Mathematical analysis
2
F
v
QvB
a
c
r
m
m
2
mv
Þ
QvB
r
mv
r
radius of motion
QB
w
v
r
BQ
rad
\
w
angular speed
angular freqency
(
)
s
m
w
BQ
f
frequency
(
cps
Hz
)
p
p
2
2
m
p
1
2
m
T
period of the motion
.
f
BQ
19Magnetic Bottles
magnetic bottles
20Magnetic Force on Current
Force on current carrying conductor in
a uniform constant magnetic field
ò
b
I
F
s
l
B
I
d
B
B
a
(
)
-
l
r
r
where
b
a
é
ù
æ
ö
ds
dQ
(
)
v
s
ç
s
dQ
dQ
ˆ
ds
ˆ
I ds
ˆ
I d
ê
ú
s
s
è
ø
ë
û
dt
dt
21Vector Integral I
ds
b
rb
B is constant
vector integral
ra
a
Current I
Want to find total force on charge as it flows
from a to b
22Vector Integral II
ds
b
rb
B
rb- ra
ra
a
I
23Vector Integral III
Sum
ds
24Magnetic Force on Current Loop I
Force on Current Loop
I
B
k
j
i
25Magnetic Force on Current Loop II
Total Force on Loop
26Torque on Current Loop I
Torque on Current Loop
??
I
B
??
k
z
??
j
i
?
??
y
27Torque on Current Loop II
28Torque on Current Loop III
29Magnetic Moment
Torque on Current Loop in yz plane in
a uniform magnetic field in positive y direction
t
k
IAB
In general the torque on a current loop in
magnetic field is
t
M
B
M
A
I
,
where
is the area vector of the loop
,
A
with the orientation given by the current flow
.
30Oriented Area Vector
AAi Area vector with orientation
I
k
A
j
i
31Hall Effect
I
Hall Effect
A
t
d
vd
FE
FB
B
V
E
-
32Mathematical analysis
At Equilibrium
F
F
E
B
V
E
d
F
F
eE
v
eB
E
B
d
E
\
v
d
B
J
I
Remember
v
d
ne
neA
I
E
BI
BI
BI
\
Þ
n
V
neA
B
EAe
Vte
dte
d
33Measurement
can measure vd by measuring the PD V.
34Lorentz Force