A copper wire has a diameter \(d_{\mathrm{Cu}}=0.0500 \mathrm{~cm}\) is \(3.00 \mathrm{~m}\) long, and has a density of charge carriers of \(8.50 \cdot 10^{28}\) electrons \(/ \mathrm{m}^{3}\). As shown in the figure, the copper wire is attached to an equal length of aluminum wire with a diameter \(d_{\mathrm{A} \mathrm{I}}=0.0100 \mathrm{~cm}\) and density of charge carriers of \(6.02 \cdot 10^{28}\) electrons \(/ \mathrm{m}^{3}\). A current of 0.400 A flows through the copper wire. a) What is the ratio of the current densities in the two wires, \(J_{\mathrm{Cu}} / J_{\mathrm{Al}} ?\) b) What is the ratio of the drift velocities in the two wires, \(v_{\mathrm{d}-\mathrm{Cu}} / v_{\mathrm{d}-\mathrm{Al}} ?\)

Short Answer

Expert verified
Using the information provided and the geometrical properties of the wires, we calculated the current density and drift velocity for both the copper and aluminum wires. We found that the ratio of the current densities in the two wires is 0.04 and the ratio of drift velocities in the two wires is 5.

Step by step solution

01

Define the given parameters for the copper and aluminum wires.

We are given the following: For Copper wire: \(d_{Cu} = 0.0500\ cm\) Length = \(3.00\ m\) Density of charge carriers = \(8.50 \times 10^{28}\ electrons/m^3\) For Aluminum wire: \(d_{Al} = 0.0100\ cm\) Length = \(3.00\ m\) Density of charge carriers = \(6.02 \times 10^{28}\ electrons/m^3\) Current flowing through copper wire = \(I_{Cu} = 0.400\ A\)
02

Calculate cross-sectional areas for the copper and aluminum wires.

To find the cross-sectional area of each wire, we use the following formula: \( A_{wire} = \pi r^2 \) For Copper wire: \(A_{Cu} = \pi (\frac{d_{Cu}}{2})^2 = \pi (\frac{0.0500\ cm}{2})^2 = \pi (\frac{0.000500\ m}{2})^2 = \pi (0.000250)^2 m^2\) For Aluminum wire: \(A_{Al} = \pi (\frac{d_{Al}}{2})^2 = \pi (\frac{0.0100\ cm}{2})^2 = \pi (\frac{0.000100\ m}{2})^2 = \pi (0.000050)^2 m^2\)
03

Calculate current densities for the copper and aluminum wires.

The current density (J) is given by: \( J = \frac{I}{A} \) For Copper wire: \(J_{Cu} = \frac{I_{Cu}}{A_{Cu}} = \frac{0.400\ A}{\pi (0.000250)^2 m^2}\) For Aluminum wire: The current flowing through the Aluminum is the same as the current in the copper wire, hence \(I_{Al} = 0.400\ A\) \(J_{Al} = \frac{I_{Al}}{A_{Al}} = \frac{0.400\ A}{\pi (0.000050)^2 m^2}\)
04

Calculate the ratio of the current densities in the two wires.

Now, we can find the ratio of the current densities: \(J_{Cu}/J_{Al} = \frac{J_{Cu}}{J_{Al}} = \frac{\frac{0.400\ A}{\pi (0.000250)^2 m^2}}{\frac{0.400\ A}{\pi (0.000050)^2 m^2}} = \frac{(0.000050)^2}{(0.000250)^2} = \frac{0.00000250}{0.0000625} = 0.04\)
05

Calculate the drift velocities for the copper and aluminum wires.

The drift velocity (v) is given by: \( v = \frac{I}{nqA} \) For Copper wire: \(v_{d-Cu} = \frac{I_{Cu}}{n_{Cu}qA_{Cu}} = \frac{0.400\ A}{(8.50 \times 10^{28}\ electrons/m^3)(1.6 \times 10^{-19}\ C)(\pi (0.000250)^2 m^2)}\) For Aluminum wire: \(v_{d-Al} = \frac{I_{Al}}{n_{Al}qA_{Al}} = \frac{0.400\ A}{(6.02 \times 10^{28}\ electrons/m^3)(1.6 \times 10^{-19}\ C)(\pi (0.000050)^2 m^2)}\)
06

Calculate the ratio of the drift velocities in the two wires.

Now, we can find the ratio of the drift velocities: \(v_{d-Cu}/v_{d-Al} = \frac{v_{d-Cu}}{v_{d-Al}} = \frac{\frac{0.400\ A}{(8.50 \times 10^{28}\ electrons/m^3)(1.6 \times 10^{-19}\ C)(\pi (0.000250)^2 m^2)}}{\frac{0.400\ A}{(6.02 \times 10^{28}\ electrons/m^3)(1.6 \times 10^{-19}\ C)(\pi (0.000050)^2 m^2)}}\) \(v_{d-Cu}/v_{d-Al} = \frac{(0.000050)^2(6.02 \times 10^{28}\ electrons/m^3)}{(0.000250)^2(8.50 \times 10^{28}\ electrons/m^3)} = 5\) So, the ratio of the current densities in the two wires is \(0.04\) and the ratio of the drift velocities in the two wires is \(5\).

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