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Nine copper wires of length \(l\) and diameter \(d\) are connected in parallel to form a single composite conductor of resistance \(R .\) What must be the diameter \(D\) of a single copper wire of length \(l\) if it is to have the same resistance?

Short Answer

Expert verified
The diameter of the single wire must be 3 times the diameter of one original wire.

Step by step solution

01

Understand Parallel Resistance Formula

When resistors are in parallel, the total resistance \(R_t\) is given by \\[\frac{1}{R_t} = \frac{1}{R_1} + \frac{1}{R_2} + \cdots + \frac{1}{R_n}\] In this case, there are 9 identical resistors (wires) each with resistance \(R_w\) and total resistance \(R\).
02

Resistance of a Single Wire

The resistance \(R\) of a wire is given by \\[R = \frac{\rho l}{A}\] \where \(\rho\) is the resistivity, \(l\) is the length, and \(A\) is the cross-sectional area. For a wire with diameter \(d\), area \(A = \frac{\pi d^2}{4}\).
03

Calculate Resistance of One Wire

Substitute the expression for area into the formula for resistance: \\[R_w = \frac{\rho l}{\frac{\pi d^2}{4}} = \frac{4\rho l}{\pi d^2}\]
04

Total Resistance of Parallel Wires

For 9 wires in parallel, \\[\frac{1}{R} = 9 \times \frac{1}{R_w} = 9 \times \frac{\pi d^2}{4\rho l}\] \This simplifies to \\[R = \frac{4\rho l}{9\pi d^2}\]
05

Equivalent Single Wire Resistance

A single wire of diameter \(D\) and the same length \(l\) should have the same resistance \(R\), thus: \\[R = \frac{4\rho l}{\pi D^2}\]
06

Equate Resistances and Solve for Diameter

Since \\[\frac{4\rho l}{9\pi d^2} = \frac{4\rho l}{\pi D^2}\] \we simplify to find: \\[9\pi d^2 = \pi D^2\] \[D^2 = 9d^2\] \[D = 3d\]
07

Final Solution Overview

The diameter \(D\) of the single copper wire must be \(3d\) to have the same resistance as the nine wires connected in parallel.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Parallel Circuits
In a parallel circuit, multiple paths allow electric current to pass through. This configuration is commonly used to ensure that if one component fails, the rest continue to function.
For resistors, or in this case, copper wires connected in a parallel circuit, the total resistance decreases. When wires are parallel, each wire shares the load, effectively reducing the overall resistance of the system.
The formula for calculating the total resistance in a parallel circuit is:
  • \(\frac{1}{R_t} = \frac{1}{R_1} + \frac{1}{R_2} + \cdots + \frac{1}{R_n}\)

This means that the more wires you add, the lower the composite resistance becomes. In our exercise, we have nine wires, which increases the overall current-tolerating capacity while keeping the voltage the same across all branches.
Resistivity
Resistivity is a fundamental property of materials that describes how strongly a material opposes the flow of electric current. It is denoted by \(\rho\) and is measured in ohm-meters (Ω·m).
Low resistivity means a material allows electric current to pass through easily. Metals like copper, which is used in the exercise, have low resistivity. This makes them excellent conductors of electricity.
Resistivity plays a critical role in determining the resistance of a wire through the formula:
  • \(R = \frac{\rho l}{A}\)

Here, \(R\) is resistance, \(l\) is the length of the wire, and \(A\) is the cross-sectional area. Understanding this relationship is key to solving problems involving wire resistance calculations, like the one we reviewed.
Cross-Sectional Area
The cross-sectional area of a wire, usually represented as \(A\), is crucial in determining its resistance. The larger the cross-sectional area, the lower the resistance, given that resistivity and length remain constant.
In our exercise, the cross-sectional area of a wire with a circular cross-section is calculated through the formula:
  • \(A = \frac{\pi d^2}{4}\)

Where \(d\) is the diameter of the wire. A wire's diameter is directly proportional to its cross-sectional area and has a significant impact on the wire's ability to conduct current.
This relationship works inversely with resistance: as area increases, resistance decreases, and vice versa. This explains why, in our exercise, increasing the diameter of the single wire to \(3d\) is necessary to match the resistance of the parallel circuit of nine wires.
Copper Wire
Copper wire is a staple in electrical engineering due to its excellent conductivity. This makes copper an ideal choice for applications needing to minimize energy loss due to resistance.
In the exercise, we explored copper wires arranged in parallel to form a composite conductor, emphasizing their superior conductive properties.
Key reasons copper is preferred:
  • Low resistivity, ensuring minimal energy loss.
  • Strong and flexible, suited for a range of applications.
  • Resistant to corrosion, increasing longevity.
Copper’s benefits translate directly into efficient and reliable performance in electrical systems, which is why it is widely used in wiring setups globally.

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Most popular questions from this chapter

The starting motor of a car is turning too slowly, and the mechanic has to decide whether to replace the motor, the cable, or the battery. The car's manual says that the \(12 \mathrm{~V}\) battery should have no more than \(0.020 \Omega\) internal resistance, the motor no more than \(0.200 \Omega\) resistance, and the cable no more than \(0.040 \Omega\) resistance. The mechanic turns on the motor and measures \(11.4 \mathrm{~V}\) across the battery, \(3.0 \mathrm{~V}\) across the cable, and a current of \(50 \mathrm{~A}\). Which part is defective?

A capacitor with an initial potential difference of \(100 \mathrm{~V}\) is discharged through a resistor when a switch between them is closed at \(t=0 .\) At \(t=10.0 \mathrm{~s}\), the potential difference across the capacitor is \(1.00 \mathrm{~V}\). (a) What is the time constant of the circuit? (b) What is the potential difference across the capacitor at \(t=17.0 \mathrm{~s}\) ?

Figure 27-64 shows the circuit of a flashing lamp, like those attached to barrels at highway construction sites. The fluorescent lamp L (of negligible capacitance) is connected in parallel across the capacitor \(C\) of an \(R C\) circuit. There is a current through the lamp only when the potential difference across it rcaches the hreakdown voltage \(V_{L}\); then the capacitor discharges completely through the lamp and the lamp flashes briefly. For a lamp with breakdown voltage \(V_{\mathrm{L}}=72.0 \mathrm{~V}\), wired to a \(95.0 \mathrm{~V}\) ideal battery and a \(0.150 \mu \mathrm{F}\) capacitor, what resistance \(R\) is needed for two flashes per second?

What multiple of the time constant \(\tau\) gives the time taken by an initially uncharged capacitor in an \(R C\) serics circuit to be charged to \(99.0 \%\) of its final charge?

Four \(18.0 \Omega\) resistors are connected in parallel across a \(25.0 \mathrm{~V}\) ideal battery. What is the current through the battery?

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