Title: phy202_5
1Lesson 5
Lesson 5
Current and Resistance
- Batteries
- Current Density
- Electron Drift Velocity
- Conductivity and Resistivity
- Resistance and Ohms Law
- Temperature Variation of Resistance
- Electrical Power and Joules Law
- Classical Model of Conduction in Metals
2Electrical Resistance
- Electrical Resistance is
- friction to the flow of electric charge
- Observed in Conductors and
- Non Conductors
- Not found in Super Conductors
3Charge Pump I
Capacitor will send current through load
resistance and loose charge
Load Resistance
I
-
4Charge Pump I
Battery will send current through load
resistance and not loose charge
Charge in battery is regenerated by Chemical
reactions
Load Resistance
I
-
5Flow of Charge
6Current Picture
I
7Current Picture Definition I
Current is the rate of Flow of positive charge
through whole cross sectional area of conductor
8Current Picture Definition II
9Conservation of Current
Current is Conserved
I1
I1I2
I2
I1
10Driving force for Current
- Flowing charge experiences friction
- Work must be done to overcome friction
- Need driving force, hence need
- Electric Field
- Potential Difference
11SI units
Potential Difference
Electrical Resistance
Current
V
R
I
V
V
W
R
(
Ohm
)
I
A
12V-I plots
I-V plots
slope constant 1/R
slope not constant
I
I
V
V
Ohmic Material
Non Ohmic Material
13Resistance I
Ohmic Materials
V
RI
Ohms
Law
V
R
constant
I
14Resistance II
Non Ohmic Materials
R is not Constant, but varies with current and
voltage
15Power
Power rate of doing work by applied force
dU
dQ
Power
V
IV
dt
dt
C
Nm
Nm
Power
I
V
AV
s
C
s
J
)
W
(
Watts
s
16Ohmic Materials I
17Ohmic Materials II
For Ohmic Materials
- Resistance is proportional to length of
conductor - Resistance is inversely proportional to the
cross sectional area of the conductor
18Resistivity
19Picture
l
I
a
V-
V
E
20Current Density
-
V
V
V
El
-
V
El
Ea
I
l
r
R
r
a
Divide by Area Current Density magnitude
Current per cross sectional area
I
E
J
s
E
r
a
1
s
conductivity
r
21Integral Formula
22Electrical Conduction
Classical Microscopic Theory of Electrical
Conduction
23Random Walk
24Picture
25Definition of Variables
Charge in Volume
D
V
D
Q
nA
x q
nAv
t q
D
D
d
n
number of charge carriers
per unit volume
A
cross sectional area
q
amount of charge on
each carrier
D
x
average distance moved in
D
time
t
after collision
v
drift velocity
d
26Equations I
D
Q
D
x
nA
q
D
t
D
t
dQ
q
Þ
I
nAv
dt
d
Þ
J
nv
q
d
J
Þ
v
nq
d
27Equations II
acceleration of charge
q
in field
E
q
a
E
m
average time between collisions
- at each collision charge carrier
forgets
drift velocity
,
so we can take initial drift
\
velocity
0
and
just before collisions
æ
ö
q
q
t
t
t
ç
v
a
E
E
è
ø
d
m
m
J
q
t
v
E
d
nq
m
2
t
nq
Þ
J
E
m
2
t
nq
Þ
s
m
28Temperature Effects
Temperature Effects
1
m
r
s
nq
t
2
As temperature increases
t
decreases
thus
r
increases
(
)
(
)
r
T
r
1
a
T
-
T
0
0
1
d
r
a
Temperature Coefficient of Resistivity
r
dT
0
29Temperature Effects
(
)
(
)
r
T
r
1
a
T
-
T
0
0
1
d
r
a
Temperature Coefficient of Resistivity
r
dT
Equation
0
Thus
(
)
(
)
a
-
T
T
R
T
R
1
0
0