The most common material used for sandpaper, silicon carbide, is also widely used in electrical applications. One common device is a tubular resistor made of a special grade of silicon carbide called carborundum. A particular carborundum resistor (see the figure) consists of a thick-walled cylindrical shell (a pipe) of inner radius \(a=\) \(1.50 \mathrm{~cm},\) outer radius \(b=2.50 \mathrm{~cm},\) and length \(L=60.0 \mathrm{~cm} .\) The resistance of this carborundum resistor at \(20 .{ }^{\circ} \mathrm{C}\) is \(1.00 \Omega\). a) Calculate the resistivity of carborundum at room temperature. Compare this to the resistivities of the most commonly used conductors (copper, aluminum, and silver). b) Carborundum has a high temperature coefficient of resistivity: \(\alpha=2.14 \cdot 10^{-3} \mathrm{~K}^{-1} .\) If, in a particular application, the carborundum resistor heats up to \(300 .{ }^{\circ} \mathrm{C},\) what is the percentage change in its resistance between room temperature \(\left(20 .{ }^{\circ} \mathrm{C}\right)\) and this operating temperature?

Short Answer

Expert verified
Answer: The resistivity of carborundum at room temperature is approximately \(7.04 \cdot 10^{-3} \Omega\text{m}\). It has a much higher resistivity compared to common conductors such as copper, aluminum, and silver. The resistance of the carborundum resistor increases by approximately 59.9% when its temperature increases from 20°C to 300°C.

Step by step solution

01

Calculate the resistivity of carborundum at room temperature

To calculate the resistivity, we can use the formula: \(\text{Resistance} = \dfrac{\rho \cdot \text{Length}}{\text{Cross-sectional area}}\) The cross-sectional area of our cylindrical resistor can be expressed as the difference between the outer circle's area and the inner circle's area: \(\text{Cross-sectional area} = \pi(b^2 - a^2)\) Now we can rearrange the resistivity formula to find \(\rho\): \(\rho = \dfrac{\text{Resistance} \cdot \text{Cross-sectional area}}{\text{Length}}\) Plug in the values given in the problem statement: \(\rho = \dfrac{1.00 \Omega \cdot \pi(2.50^2 - 1.50^2)}{60.0}\) Calculate the resistivity: \(\rho \approx 7.04 \cdot 10^{-3} \text{ }\Omega\text{m}\)
02

Compare the resistivity of carborundum to common conductors

Let's compare the resistivity of carborundum (\(7.04 \cdot 10^{-3} \Omega\text{m}\)) to some common conductors: - Copper: \(\rho_{Cu} \approx 1.68 \cdot 10^{-8} \Omega\text{m}\) - Aluminum: \(\rho_{Al} \approx 2.82 \cdot 10^{-8} \Omega\text{m}\) - Silver: \(\rho_{Ag} \approx 1.59 \cdot 10^{-8} \Omega\text{m}\) Carborundum has a much higher resistivity compared to these common conductors, which is why it is used for resistive applications rather than conductive applications.
03

Calculate the percentage change in resistance

We can find the percentage change in resistance between the room temperature and the operating temperature using the formula: \(\Delta R (\%) = \alpha \cdot \Delta T \cdot 100\) Where \(\Delta R (\%)\) is the percentage change in resistance, \(\alpha = 2.14 \cdot 10^{-3} \mathrm{~K}^{-1}\) is the temperature coefficient of resistivity, and \(\Delta T\) is the temperature difference. The temperature difference is: \(\Delta T = 300^{\circ}C - 20^{\circ}C = 280^{\circ}C = 280\text{ K}\) Now find the percentage change in resistance: \(\Delta R(\%) = 2.14 \cdot 10^{-3} \mathrm{~K}^{-1} \cdot 280 \text{ K} \cdot 100\) \(\Delta R(\%) \approx 59.9 \%\) The resistance of the carborundum resistor increases by approximately \(59.9\%\) when its temperature increases from \(20^{\circ}C\) to \(300^{\circ}C\).

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Most popular questions from this chapter

Should light bulbs (ordinary incandescent bulbs with tungsten filaments) be considered ohmic resistors? Why or why not? How would this be determined experimentally?

Before bendable tungsten filaments were developed, Thomas Edison used carbon filaments in his light bulbs. Though carbon has a very high melting temperature \(\left(3599^{\circ} \mathrm{C}\right)\) its sublimation rate is high at high temperatures. So carbonfilament bulbs were kept at lower temperatures, thereby rendering them dimmer than later tungsten-based bulbs. A typical carbon-filament bulb requires an average power of \(40 \mathrm{~W}\), when 110 volts is applied across it, and has a filament temperature of \(1800^{\circ} \mathrm{C}\). Carbon, unlike copper, has a negative temperature coefficient of resistivity: \(\alpha=-0.0005^{\circ} \mathrm{C}^{-1}\) Calculate the resistance at room temperature \(\left(20^{\circ} \mathrm{C}\right)\) of this carbon filament.

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The resistivity of a conductor is \(\rho=1.00 \cdot 10^{-5} \Omega \mathrm{m}\). If a cylindrical wire is made of this conductor, with a crosssectional area of \(1.00 \cdot 10^{-6} \mathrm{~m}^{2},\) what should the length of the wire be for its resistance to be \(10.0 \Omega ?\)

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