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R = R 0 ( 1 + α Δ T )

is the temperature dependence of the resistance of an object, where R 0 is the original resistance (usually taken to be 20.00 ° C ) and R is the resistance after a temperature change Δ T . The color code gives the resistance of the resistor at a temperature of T = 20.00 ° C .

Numerous thermometers are based on the effect of temperature on resistance ( [link] ). One of the most common thermometers is based on the thermistor, a semiconductor crystal with a strong temperature dependence, the resistance of which is measured to obtain its temperature. The device is small, so that it quickly comes into thermal equilibrium with the part of a person it touches.

Picture is a photograph of two digital oral thermometers.
These familiar thermometers are based on the automated measurement of a thermistor’s temperature-dependent resistance.

Calculating resistance

Although caution must be used in applying ρ = ρ 0 ( 1 + α Δ T ) and R = R 0 ( 1 + α Δ T ) for temperature changes greater than 100 ° C , for tungsten, the equations work reasonably well for very large temperature changes. A tungsten filament at 20 ° C has a resistance of 0.350 Ω . What would the resistance be if the temperature is increased to 2850 ° C ?

Strategy

This is a straightforward application of R = R 0 ( 1 + α Δ T ) , since the original resistance of the filament is given as R 0 = 0.350 Ω and the temperature change is Δ T = 2830 ° C .

Solution

The resistance of the hotter filament R is obtained by entering known values into the above equation:

R = R 0 ( 1 + α Δ T ) = ( 0.350 Ω ) [ 1 + ( 4.5 × 10 −3 ° C ) ( 2830 ° C ) ] = 4.8 Ω .

Significance

Notice that the resistance changes by more than a factor of 10 as the filament warms to the high temperature and the current through the filament depends on the resistance of the filament and the voltage applied. If the filament is used in an incandescent light bulb, the initial current through the filament when the bulb is first energized will be higher than the current after the filament reaches the operating temperature.

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Check Your Understanding A strain gauge is an electrical device to measure strain, as shown below. It consists of a flexible, insulating backing that supports a conduction foil pattern. The resistance of the foil changes as the backing is stretched. How does the strain gauge resistance change? Is the strain gauge affected by temperature changes?

Picture is a schematic drawing of a strain gauge device that consists of the conducting pattern deposited on the insulated surface. Metal contacts are made to the two large pads at the origin of the conducting pattern.

The foil pattern stretches as the backing stretches, and the foil tracks become longer and thinner. Since the resistance is calculated as R = ρ L A , the resistance increases as the foil tracks are stretched. When the temperature changes, so does the resistivity of the foil tracks, changing the resistance. One way to combat this is to use two strain gauges, one used as a reference and the other used to measure the strain. The two strain gauges are kept at a constant temperature

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The resistance of coaxial cable

Long cables can sometimes act like antennas, picking up electronic noise, which are signals from other equipment and appliances. Coaxial cables are used for many applications that require this noise to be eliminated. For example, they can be found in the home in cable TV connections or other audiovisual connections. Coaxial cables consist of an inner conductor of radius r i surrounded by a second, outer concentric conductor with radius r o ( [link] ). The space between the two is normally filled with an insulator such as polyethylene plastic. A small amount of radial leakage current occurs between the two conductors. Determine the resistance of a coaxial cable of length L .

Picture is a schematic drawing of a coaxial cable. It consists of a central metal core encapsulated by the dielectric insulator. Metal shield surrounds dielectric insulator. The whole assembly in inserted in the plastic jacket.
Coaxial cables consist of two concentric conductors separated by insulation. They are often used in cable TV or other audiovisual connections.

Strategy

We cannot use the equation R = ρ L A directly. Instead, we look at concentric cylindrical shells, with thickness dr , and integrate.

Solution

We first find an expression for dR and then integrate from r i to r o ,

d R = ρ A d r = ρ 2 π r L d r , R = r i r o d R = r i r o ρ 2 π r L d r = ρ 2 π L r i r o 1 r d r = ρ 2 π L ln r o r i .

Significance

The resistance of a coaxial cable depends on its length, the inner and outer radii, and the resistivity of the material separating the two conductors. Since this resistance is not infinite, a small leakage current occurs between the two conductors. This leakage current leads to the attenuation (or weakening) of the signal being sent through the cable.

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Practice Key Terms 4

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Source:  OpenStax, University physics volume 2. OpenStax CNX. Oct 06, 2016 Download for free at http://cnx.org/content/col12074/1.3
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