Chapter 3
Resistance

Resistance of Conductors
Resistance of material is dependent on several factors:
Type of Material
Length of the Conductor
Cross-sectional area
Temperature

Type of Material
Atomic differences of materials cause variations in how electron collisions affect resistance
Differences produce resistivity

Type of Material
Represented by the symbol r
(Greek letter rho)
Units of r
Ohms x meters (Ω∙m) or (circular mils x ohms)/feet (Ω∙CM/ft)

Length
Resistance of a conductor
Directly proportional to its length
If you double the length of the wire, the resistance will double
 l = length
In meters or feet

Area
Resistance of a conductor
Inversely proportional to cross-sectional area of the conductor
If cross-sectional area is doubled
Resistance will be one half as much

Area
A =
Cross-sectional area, in m2 or circular mils (CM)

Resistance Formula
At a given temperature (usually 20 o C)
Formula can be used with both circular and rectangular conductors

Electrical Wire Tables
American Wire Gauge is primary system to denote wire diameters
The higher the AWG number, the smaller the diameter

Electrical Wire Tables
A given length of AWG 22 wire will have more resistance than the same length of AWG 14 wire
Larger gauge wires can handle more current

Circular Mils (CM)
Length may also be in mils (0.001 inch)
Area may be in circular mils (CM)
1 CM
Area of a circle having a diameter of 1 mil

Circular Mils (CM)
1 square mil
Area of a square having sides of 1 mil
1 CM =
p/4 square mils

Temperature Effects
For most conductors, a temperature increase causes an increase in resistance
Increase is relatively linear
In semiconductors and insulators
Increase in temperature results in decrease in resistance

Temperature Effects
Any material for which the resistance increases with temperature is said to have a positive temperature coefficient
If it decreases, it has a negative coefficient

Temperature Effects
Temperature coefficient
Rate of change of resistance with respect to temperature
It is represented by a (Greek letter alpha)

Temperature Effects
Resistance at a specific temperature (R) may be calculated from resistance at a different temperature (R1) by the formula:

Temperature Effects
Where ΔT =
T – T1 is the difference between the two temperatures in Celsius degrees

Fixed Resistors
Resistance of a fixed resistor is constant over a wide temperature range
Rated by amount of resistance
Measured in ohms (Ω)
Also rated by power
Measured in watts (W)

Fixed Resistors
Different resistors for different applications
Molded carbon composition
Carbon film
Metal film
Metal Oxide
Wire-Wound
Integrated circuit packages

Variable Resistors
Resistance may be changed (varied)
Adjust volume, set level of lighting, adjust temperature
Have three terminals
Center terminal connected to wiper arm
Potentiometers
Rheostats

Color Code
Colored bands on a resistor provide a code for determining
Value
Tolerance
Reliability

Measuring Resistance
Ohmmeter
Remove all power sources to circuit
Isolate component
Connect probes across component
No need to worry about polarity
Ohmmeter determines shorts and opens

Thermistors
Two-terminal transducer
Resistance changes with temperature
Applications include electronic thermometers and thermostatic control circuits for furnaces

Thermistors
Most have negative temperature coefficients

Photoconductive Cells
Two-terminal transducers
Resistance determined by amount of light
May be used to measure light intensity or to control lighting
Used in security systems
Linear response (negative slope)

Diodes
Semiconductor devices
Conduct in one direction only
In forward direction, has very little resistance
In reverse direction, resistance is very high
Open circuit

Varistors
Resistors sensitive to voltage
High resistance when voltage is below breakdown value
Low resistance when voltage is above breakdown value
High power ratings
When used in surge protectors

Conductance
Measure of a material’s ability to allow flow of electrical current
Conductance is reciprocal of resistance
G = 1/R
Unit is siemens (S)

Superconductors
Low temperatures
Resistance of some materials goes to almost zero
Temperature is called critical temperature

Superconductors
Meissner Effect
Cooled below its critical temperature
Magnetic fields may surround but not enter the superconductor