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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 cross-sectional area of \(1.00 \cdot 10^{-6} \mathrm{~m}^{2}\) what should the length of the wire be for its resistance to be \(10.0 \Omega ?\)

Short Answer

Expert verified
Answer: The required length of the wire is \(1.00 \mathrm{m}\).

Step by step solution

01

Identify the given information

We are given the following information: - Resistivity, \(\rho = 1.00 \cdot 10^{-5} \Omega \mathrm{m}\) - Cross-sectional area, \(A = 1.00 \cdot 10^{-6} \mathrm{~m}^{2}\) - Resistance, \(R = 10.0 \Omega\)
02

Recall the formula for resistance

The formula for resistance in terms of resistivity, cross-sectional area, and length is given by: \(R = \frac{\rho L}{A}\) Where: - \(R\) is the resistance - \(\rho\) is the resistivity - \(L\) is the length of the wire - \(A\) is the cross-sectional area
03

Rearrange the formula to solve for length

We need to find the length of the wire, so we will rearrange the formula to isolate \(L\): \(L = \frac{R \times A}{\rho}\)
04

Substitute the given values into the formula

Plug the given values for resistance, area, and resistivity into the formula: \(L = \frac{10.0 \Omega \times 1.00 \cdot 10^{-6} \mathrm{~m}^{2}}{1.00 \cdot 10^{-5} \Omega \mathrm{m}}\)
05

Calculate the length

Simplify the equation to find the length of the wire required: \(L = \frac{10.0 \times 1.00 \cdot 10^{-6}}{1.00 \cdot 10^{-5}} = 1.00 \mathrm{m}\) The length of the wire should be \(1.00\mathrm{m}\) for its resistance to be \(10.0 \Omega\).

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Most popular questions from this chapter

The Stanford Linear Accelerator accelerated a beam consisting of \(2.0 \cdot 10^{14}\) electrons per second through a potential difference of \(2.0 \cdot 10^{10} \mathrm{~V}\) a) Calculate the current in the beam. b) Calculate the power of the beam. c) Calculate the effective ohmic resistance of the accelerator.

A 34-gauge copper wire \(\left(A=0.0201 \mathrm{~mm}^{2}\right),\) with a constant potential difference of \(0.100 \mathrm{~V}\) applied across its \(1.00 \mathrm{~m}\) length at room temperature \(\left(20.0^{\circ} \mathrm{C}\right),\) is cooled to liquid nitrogen temperature \(\left(77 \mathrm{~K}=-196^{\circ} \mathrm{C}\right)\) a) Determine the percentage change in the wire's resistance during the drop in temperature. b) Determine the percentage change in current flowing in the wire. c) Compare the drift speeds of the electrons at the two temperatures.

If the current through a resistor is increased by a factor of \(2,\) how does this affect the power that is dissipated? a) It decreases by a factor of 4 . b) It increases by a factor of 2 . c) It decreases by a factor of 8 . d) It increases by a factor of 4 .

Two cylindrical wires, 1 and 2 , made of the same material, have the same resistance. If the length of wire 2 is twice that of wire \(1,\) what is the ratio of their cross-sectional areas, \(A_{1}\) and \(A_{2} ?\) a) \(A_{1} / A_{2}=2\) c) \(A_{1} / A_{2}=0.5\) b) \(A_{1} / A_{2}=4\) d) \(A_{1} / A_{2}=0.25\)

A material is said to be ohmic if an electric field, \(\vec{E}\), in the material gives rise to current density \(\vec{J}=\sigma \vec{E},\) where the conductivity, \(\sigma\) is a constant independent of \(\vec{E}\) or \(\bar{J}\). (This is the precise form of Ohm's Law, ) Suppose in some material an electric field, \(\vec{E}\), produces current density, \(\bar{J},\) not necessarily related by Ohm's Law; that is, the material may or may not be ohmic. a) Calculate the rate of energy dissipation (sometimes called ohmic heating or joule heating) per unit volume in this material, in terms of \(\vec{E}\) and \(\vec{J}\). b) Express the result of part (a) in terms of \(\vec{E}\) alone and \(\vec{J}\) alone, for \(\overrightarrow{\boldsymbol{E}}\) and \(\vec{J}\) related via Ohm's Law, that is, in an ohmic material with conductivity \(\sigma\) or resistivity \(\rho\).

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