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Make a Generator? You are shipwrecked on a deserted tropical island. You have some electrical devices that you could operate using a generator but you have no magnets. The earth's magnetic field at your location is horizontal and has magnitude \(8.0 \times 10^{-5} \mathrm{T},\) and you decide to try to use this field for a generator by rotating a large circular coil of wire at a high rate. You need to produce a peak emf of 9.0 \(\mathrm{V}\) and estimate that you can rotate the coil at 30 \(\mathrm{rpm}\) by turning a crank handle. You also decide that to have an acceptable coil resistance, the maximum number of turns the coil can have is 2000 . (a) What area must the coil have? (b) If the coil is circular, what is the maximum translational speed of a point on the coil as it rotates? Do you think this device is feasible? Explain.

Short Answer

Expert verified
Area should be 17.9 m²; edge speed is 7.54 m/s. Device is impractical.

Step by step solution

01

Understanding the Problem

We are tasked with finding the area of a coil needed to generate a peak emf of 9.0 V using the Earth's horizontal magnetic field. The coil rotates at 30 rpm, and we can have up to 2000 turns in the coil. Later, we'll find the maximum speed of a point on the coil.
02

Formula for Peak EMF

The peak electromotive force (emf) in a coil rotating in a magnetic field is given by the formula \( \epsilon = NAB\omega \), where \( N \) is the number of turns, \( A \) is the area of the coil, \( B \) is the magnetic field strength, and \( \omega \) is the angular speed in radians per second.
03

Converting RPM to Radians Per Second

The angular speed \( \omega \) in radians per second is given by \( \omega = \frac{2\pi \times \, \text{rpm}}{60} \). Thus, for 30 rpm, we calculate \( \omega = \frac{2\pi \times 30}{60} = \pi \) rad/s.
04

Solving for Area A

Re-arrange the peak emf formula to solve for the area \( A \) \[ \epsilon = NAB\omega \Rightarrow A = \frac{\epsilon}{NB\omega} \]. Using the given values: \( \epsilon = 9.0 \text{V}, N = 2000, B = 8.0 \times 10^{-5} \text{T}, \omega = \pi \), we have \( A = \frac{9}{2000 \times 8.0 \times 10^{-5} \times \pi} \approx 17.9 \text{ m}^2 \).
05

Translational Speed at Coil's Edge

The maximum translational speed \( v \) of a point on the edge of a rotating disc is given by \( v = r\omega \), where \( r \) is the radius of the coil. First, find the radius \( r = \sqrt{\frac{A}{\pi}} \), then use it to find \( v \). Calculate \( r = \sqrt{\frac{17.9}{\pi}} \approx 2.4 \text{ m} \) so \( v = 2.4 \times \pi \approx 7.54 \text{ m/s} \).
06

Evaluating Feasibility

Considering the coil area is large (17.9 square meters) which exceeds typical practical constraints for a coil meant for human crank operation, and the edge speed of 7.54 m/s (about 27 km/h) might be difficult to maintain manually, suggests this setup is highly impractical on the island.

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Key Concepts

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

Faraday's Law of Induction
Faraday's Law of Induction is a fundamental principle in electromagnetism that explains how electric fields are generated by changing magnetic fields. This law forms the basis for understanding how generators work. The law states that the electromotive force (emf) generated is equal to the negative rate of change of magnetic flux through a circuit. In simpler terms, it describes how moving a coil in a magnetic field or changing the magnetic field across a coil produces electricity.

In our generator scenario, Faraday's Law governs the creation of electricity by rotating a coil in the Earth's magnetic field. The formula used, \( \epsilon = NAB\omega \), ties together the number of turns in the coil \( N \), the coil area \( A \), the magnetic field strength \( B \), and the angular speed \( \omega \) to find the peak emf \( \epsilon \). By understanding and using these variables, you can predict how much electricity your generator can create.
Generator Design
The concept of generator design is crucial when you want to transform mechanical energy into electrical energy. In designing your generator on the island, the key elements include the coil of wire, the magnetic field, and motion provided by your crank.

To maximize the efficiency of this design, the number of turns in the coil and the coil’s area both play vital roles. More turns in the coil help amplify the potential electricity generated. However, there's a limit to the resistance a coil can tolerate, affecting its efficiency. On the island, you're limited to a maximum of 2000 turns. Working within this constraint while achieving the desired peak emf involves careful engineering calculations.

The design must ensure that it is practical and feasible to produce sufficient electricity with available resources and under given conditions. Crafting such a generator from scratch is a helpful exercise in applying physics principles logically.
Angular Speed
Angular speed, symbolized as \( \omega \), is a measure of how fast an object is rotating. It's a critical factor in the functionality of your island generator. It's expressed in radians per second and is calculated by converting revolutions per minute (rpm) to this unit. The formula \( \omega = \frac{2\pi \times \ \text{rpm}}{60} \) simplifies this process.

For your island generator, you planned to rotate the coil at 30 rpm. Converting this to radians per second gives \( \omega = \pi \ \text{rad/s}\). This value is used in Faraday's Law to determine how efficiently you can transform the mechanical energy from cranking into electrical energy. The faster the rotation, the higher the potential for electricity generation. However, practical limits, like human endurance for cranking, must be considered.
Coil Resistance
Coil resistance is an important aspect to consider in the design of any generator. This resistance is determined largely by the material of the wire, the coil's length, and its thickness. It directly influences how much current the coil can carry without losing energy to heat.

In the scenario, setting a limit of 2000 turns was partly to manage the resistance level. Higher resistance reduces overall efficiency by converting useful electric energy into heat. So, while more turns in the coil may increase the generated voltage, too many turns can increase the resistance, diminishing returns in terms of usable power.

Balancing the number of coil turns with design constraints is key to creating an effective generator. A coil that has too high resistance will prevent reaching the desired peak emf of 9.0 V needed to power devices, which is crucial in a survival situation.

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Most popular questions from this chapter

The armature of a small generator consists of a flat, square coil with 120 turns and sides with a length of 1.60 \(\mathrm{cm} .\) The coil rotates in a magnetic field of 0.0750 T. What is the angular speed of the coil if the maximum emf produced is 24.0 \(\mathrm{mV}\) ?

CALC A very long, straight solenoid with a cross-sectional area of 2.00 \(\mathrm{cm}^{2}\) is wound with 90.0 turns of wire per centimeter. Starting at \(t=0,\) the current in the solenoid is increasing according to \(i(t)=\left(0.160 \mathrm{A} / \mathrm{s}^{2}\right) t^{2}\) . A secondary winding of 5 turns encircles the solenoid at its center, such that the secondary winding has the same cross-sectional area as the solenoid. What is the magnitude of the emf induced in the secondary winding at the instant that the current in the solenoid is 3.20 \(\mathrm{A}\) ?

A metal ring 4.50 \(\mathrm{cm}\) in diameter is placed between the north and south poles of large magnets with the plane of its area perpendicular to the magnetic field. These magnets produce an initial uniform field of 1.12 T between them but are gradually pulled apart, causing this field to remain uniform but decrease steadily at 0.250 \(\mathrm{T} / \mathrm{s}\) (a) What is the magnitude of the electric field induced in the ring? (b) In which direction (clockwise or counterclockwise) does the current flow as viewed by someone on the south pole of the magnet?

Back emf. A motor with a brush-and-commutator arrangement, as described in Example \(29.4,\) has a circular coil with radius 2.5 \(\mathrm{cm}\) and 150 turns of wire. The magnetic field has magnitude \(0.060 \mathrm{T},\) and the coil rotates at 440 \(\mathrm{rev} / \mathrm{min.}\) (a) What is the maximum emf induced in the coil? (b) What is the average back emf?

The compound \(\mathrm{SiV}_{3}\) is a type-II superconductor. At temperatures near absolute zero the two critical fields are \(B_{\mathrm{cl}}=55.0 \mathrm{mT}\) and \(B_{\mathrm{c} 2}=15.0 \mathrm{T}\) . The normal phase of \(\mathrm{Si} \mathrm{V}_{3}\) has a magnetic susceptibility close to zero. A long, thin \(\mathrm{SiV}_{3}\) cylinder has its axis parallel to an external magnetic field \(\vec{\boldsymbol{B}}_{0}\) in the \(+x\) -direction. At points far from the ends of the cylinder, by symmetry, all the magnetic vectors are parallel to the \(x\) -axis. At a temperature near absolute zero, the external magnetic field is slowly increased from zero. What are the resultant magnetic field \(\vec{\boldsymbol{B}}\) and the magnetization \(\vec{M}\) inside the cylinder at points far from its ends (a) just before the magnetic flux begins to penetrate the material, and (b) just after the material becomes completely normal?

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