1. Ohm’s “Law”: Resistance & Resistors

2. The ratio of voltage to current is called the Resistance R
Experimentally, it is often (but not always!)
found that the current I in a wire is proportional
to the potential difference V between its ends:
The ratio of voltage to current is called the Resistance R

3. SI Unit of Resistance: The Ohm, Ω: 1 Ω ≡ 1 V/A.
In many conductors, the
resistance is independent of the
voltage; this relationship is called
Ohm’s “Law”.
Note: This isn’t really a “Law”,
but a relationship that only holds
sometimes! Materials that do not
follow Ohm’s Law are called
Non-Ohmic Materials
A Non-Ohmic
System
Figure Graphs of current vs. voltage for (a) a metal conductor which obeys Ohm’s law, and (b) for a nonohmic device, in this case a semiconductor diode.
SI Unit of Resistance: The Ohm, Ω: 1 Ω ≡ 1 V/A.

4. Georg Simon Ohm: March 16, 1787 - July 7,1854
German physicist, high school teacher. Research on Volta’s
electrochemical cell. Found current flowing through a wire is proportional to
cross sectional area & inversely proportional to its length. Using this, he was able
to define the relation between voltage, current, & resistance. These relationships
are of such importance, that they represent the beginning of
electrical circuit analysis. When he published his finding in 1827, his
ideas were dismissed by his colleagues. He was forced to resign from his high
school teaching position & he lived in poverty & shame until he accepted a
position at Nüremberg in 1833.

5. A current I enters a resistor R as shown.
Conceptual Example
Current and Potential.
A current I enters a resistor R as shown.
(a) Is the potential higher at point A or at point B?
(b) Is the current greater at point A or at point B?
Solution: a. Point A is at higher potential (current flows “downhill”).
b. The current is the same – all the charge that flows past A also flows past B.

6. Flashlight Bulb Resistance.
Example
Flashlight Bulb Resistance.
A small flashlight bulb draws a current of I = 300 mA from its battery, which supplies V = 1.5 V.
(a) Calculate the resistance R of the bulb.
(b) Suppose that the battery
becomes weak so the voltage
drops to 1.2 V, Calculate the
current now.
Figure Flashlight (Example 25–4). Note how the circuit is completed along the side strip.
a. R = V/I = 5.0 Ω.
b. Assuming the resistance stays the same, the current will drop to 240 mA.

7. Standard resistors are manufactured for use in electric circuits; they are color-coded to indicate their value and precision.
Figure The resistance value of a given resistor is written on the exterior, or may be given as a color code as shown above and in the Table: the first two colors represent the first two digits in the value of the resistance, the third color represents the power of ten that it must be multiplied by, and the fourth is the manufactured tolerance. For example, a resistor whose four colors are red, green, yellow, and silver has a resistance of 25 x 104 Ω = 250,000 Ω = 250 kΩ, plus or minus 10%. An alternate example of a simple code is a number such as 104, which means R = 1.0 x 104 Ω.

8. This is the standard resistor color code
This is the standard resistor color code. Note that the colors from red to violet are in the order they appear in a rainbow.

9. Some Clarifications Current is not a vector but it does have
Batteries maintain a (nearly) constant
potential difference; the current varies.
Resistance is a property of a material or
device.
Current is not a vector but it does have
a direction.
Current and charge do not get used up.
Whatever charge goes in one end of a
circuit comes out the other end.

10. Resistivity ρ is called The Resistivity, & is
The resistance of a wire is proportional
to its length and inversely proportional
to its cross-sectional area:
ρ is called The Resistivity, & is
characteristic of the material.

11. This table gives the resistivity and temperature coefficients of typical conductors, semiconductors, and insulators.

12. Example: Speaker Wires
Suppose that you want to connect your stereo to remote speakers.
(a) If each wire must be
ℓ = 20 m long, calculate the diameter of copper wire should you use to keep the resistance R less than R = 0.10 Ω per wire.
(b) If the current to each speaker is I = 4.0 A, calculate the potential difference, or voltage drop V across each wire.
Solution: a. R = ρl/A; you can solve this for A and then find the diameter. D = 2.1 mm.
b. V = IR = 0.40 V.

13. Resistance of a Cable, Example
Coaxial Cable
Assume the plastic between the conductors to be concentric elements of thickness dr. The resistance of the hollow cylinder of plastic is obtained by starting with:

14. This is the radial resistance of the cable.
Total resistance across the entire thickness is:
This is the radial resistance of the cable.
The calculated value is fairly high, which is
desirable since you want the current to flow
along the cable and not radially out of it!!

15. Stretching changes resistance.
Conceptual Example
Stretching changes resistance.
Suppose a wire of resistance R could be stretched uniformly until it was twice its original length. What would happen to its resistance?
Solution: The total volume of the wire should stay the same; therefore if the length doubles, the cross-sectional area is halved. This increases the resistance by a factor of 4.

16. For a given material, the resistivity ρ increases with temperature:
Using the relationship between resistance R & resistivity ρ:
The temperature dependence of R becomes:
RT = R0[1 + (T – T0)]

17. Example: Resistance Thermometer.
The variation in electrical resistance with
temperature can be used to make precise
temperature measurements.
Platinum is commonly used, since it is relatively
free from corrosive effects & has a high melting point.
At T0 = 20.0°C, the resistance of a platinum
resistance thermometer is R0 = Ω.
When placed in a particular solution, the
resistance is R = Ω. Calculate the
temperature of this solution.
Solution: The resistance is proportional to the resistivity; use the temperature dependence of resistivity to find the temperature. T = 56.0 °C.

18. Electrical Power

19. Electrical Power Assume a circuit as shown. As a
charge moves from a to b, the
electric potential energy of the
system increases by QdV.
The chemical energy in the battery must decrease by this same amount.
This electric potential energy is
transformed into internal energy
in the resistor.
This corresponds to increased vibrational motion of the atoms in the resistor

20. which the energy is delivered to the resistor.
The resistor is normally in contact with the air, so
its increased temperature will result in a transfer
of energy by heat into the air.
The resistor also emits thermal radiation. After
some time interval, the resistor reaches a constant
temperature.
The input of energy from the battery is balanced by the output of energy by heat and radiation.
The rate at which the system’s potential energy
decreases as the charge passes through the resistor is
equal to the rate at which the system gains internal\
energy in the resistor. The power is the rate at
which the energy is delivered to the resistor.

21. So the power it transforms is
Power, as in kinematics, is the energy
transformed by a device per unit time:
For a current carrying circuit, potential energy is:
U = qV
So the power it transforms is or

22. The SI unit of power is the watt, W.
So, the power is given by P = IV. Applying Ohm’s “Law”, alternative expressions can be found:
The SI unit of power is the watt, W.

23. Example: Headlights.
Calculate the resistance R of a P = 40 W automobile headlight designed for V = 12 V.
Solution: R = V2/P = 3.6 Ω.

24. A side note! 1 kWh = (1000 W)(3600 s) = 3.60 x 106 J.
What you pay for on your electric bill is not power, but energy – the power consumption multiplied by the time. We have been measuring energy in Joules, but the electric company measures it in kilowatt-hours, kWh:
1 kWh = (1000 W)(3600 s)
= 3.60 x 106 J.

25. Example: Electric heater.
An electric heater draws a steady current
I = 15.0 A on a V = 120-V line. How much power does it require and how much does it cost per month (30 days) if it operates 3.0 h per day and the electric company charges 9.2 cents per kWh?
Solution: P = IV = 1800 W W x 3.0 h/day x 30 days = 162 kWh. At 9.2 cents per kWh, this would cost $15.

26. Example: Lightning Bolt
Lightning is a spectacular example of electric current
in a natural phenomenon. There is much variability to
lightning bolts, but a typical event can transfer
109 J of energy across a potential difference of perhaps V = 5 x 107 V during a time interval of about 0.2 s.
Use this information to estimate
(a) the total amount of charge transferred
between cloud and ground,
(b) the current in the lightning bolt,
(c) the average power delivered over the 0.2 s.
Solution: a. The charge is the change in energy divided by the change in electric potential: Q = 20 C.
b. I = Q/t = 100 A.
c. P = energy/time = IV = 5 x 109 W = 5 GW.

27. Power in Household Circuits
The wires used in homes to carry electricity have very low resistance.
However, if the current is high enough, the power will increase and the wires can
become hot enough to start a fire.
To avoid this, we use fuses or circuit breakers, which disconnect when the current goes
above a predetermined value.

28. Fuses are one-use items – if they blow, the fuse is destroyed and must be replaced.
Figure 25-19a. Fuses. When the current exceeds a certain value, the metallic ribbon melts and the circuit opens. Then the fuse must be replaced.

29. Circuit breakers, which are now much more common in homes than they once were, are switches that will open if the current is too high; they can then be reset.
Figure (b) One type of circuit breaker. The electric current passes through a bimetallic strip. When the current exceeds a safe level, the heating of the bimetallic strip causes the strip to bend so far to the left that the notch in the spring-loaded metal strip drops down over the end of the bimetallic strip; (c) the circuit then opens at the contact points (one is attached to the metal strip) and the outside switch is also flipped. As soon as the bimetallic strip cools down, it can be reset using the outside switch. Magnetic-type circuit breakers are discussed in Chapters 27 and 29.

30. Example: Will a fuse blow?
Calculate the total current drawn by all the devices in the circuit shown.
Solution: The current is given by I = P/V, where V = 120 V. Adding the currents gives 28.7 A, which exceeds the usual 20-A circuit breakers found in most household applications. The electric heater should probably be on its own circuit.

31. A dangerous extension cord.
Conceptual Example:
A dangerous extension cord.
Your 1800-W portable electric heater is too far from your desk to warm your feet. Its cord is too short, so you plug it into an extension cord rated at 11 A. Why is this dangerous?
Solution: An 1800-W heater operating at 120 V draws 15 A of current, which exceeds the rating of the extension cord. This creates a risk of overheating and fire.