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As a new electrical engineer for the local power company, you are assigned the project of designing a generator of sinusoidal ac voltage with a maximum voltage of 120 \(\mathrm{V}\) . Besides plenty of wire, you have two strong magnets that can produce a constant uniform magnetic field of 1.5 T over a square area of 10.0 \(\mathrm{cm}\) on a side when they are 12.0 \(\mathrm{cm}\) apart. The basic design should consist of a square coil turning in the uniform magnetic field. To have an acceptable coil resistance, the coil can have at most 400 loops. What is the minimum rotation rate (in \(\mathrm{rpm} )\) of the coil so it will produce the required voltage?

Short Answer

Expert verified
The minimum rotation rate is approximately 191 rpm.

Step by step solution

01

Understand the formulas

The maximum voltage induced in the coil is given by the formula for peak emf: \( \varepsilon_{max} = NAB \omega \sin(\theta) \). For maximum voltage when \( \theta = 90^\circ \), \( \sin(\theta) = 1 \), so we simplify to \( \varepsilon_{max} = NAB \omega \).
02

Calculate the coil area

The area \( A \) of the coil is \( A = \text{side}^2 \). Given a side length of 10.0 cm, convert this to meters: \( 0.1 \text{ m} \), so \( A = (0.1)^2 = 0.01 \text{ m}^2 \).
03

Set up the equation for \( \omega \)

Rearrange the peak emf formula \( \varepsilon_{max} = NAB \omega \) to solve for \( \omega \): \( \omega = \frac{\varepsilon_{max}}{NAB} \).
04

Substitute known values into the formula

Substitute \( \varepsilon_{max} = 120 \text{ V} \), \( N = 400 \), \( A = 0.01 \text{ m}^2 \), and \( B = 1.5 \text{ T} \) into \( \omega = \frac{\varepsilon_{max}}{NAB} \). This gives \( \omega = \frac{120}{400 \cdot 0.01 \cdot 1.5} = 20 \text{ rad/s} \).
05

Convert angular speed from rad/s to rpm

Use the conversion formula where 1 revolution = 2\( \pi \) radians and 1 minute = 60 seconds. Thus, \( \text{rpm} = \frac{20}{2\pi} \times 60 \). Calculate \( \frac{20}{2\pi} \cdot 60 \approx 191 \) rpm.

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Key Concepts

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

Faraday's Law
Faraday's Law of electromagnetic induction is a fundamental concept in physics, particularly in electromagnetism. It's key to understanding how an AC generator works. According to Faraday's Law, a change in the magnetic environment of a coil of wire will induce an electromotive force (EMF) in the coil. This change can be due to a variation in the magnetic field, the movement of the coil, or both.

In the case of an AC generator, this is achieved by rotating a coil within a magnetic field. The faster the coil rotates, the more rapidly the magnetic flux changes, which increases the induced EMF. This is precisely why we manipulate the rotation rate to achieve a desired voltage, as you'll notice in AC generator design exercises.

Key aspects to remember include:
  • EMF is directly proportional to the rate of change of magnetic flux.
  • The direction of the induced EMF is given by Lenz's Law, which states that the induced EMF will always work to oppose the change in flux.
This law is essential for creating efficient generators and is foundational knowledge for electrical engineering.
Electromagnetic Induction
Electromagnetic induction is the process by which a conductor placed in a changing magnetic field causes the production of voltage across the conductor. This happens because the external magnetic field enables the free electrons in the conductor to flow, or it moves the whole conductor in a magnetic field, creating a current.

This principle is the heart of many electrical appliances and applications, including generators. In the context of a generator, when the coil of wire spins in the magnetic field, the magnetic lines of force are cut by the coil, which induces an electromotive force (EMF) and generates an alternating current (AC).

Important points of electromagnetic induction involve:
  • The number of coils involved affects the magnitude of the induced voltage.
  • The strength of the magnetic field also significantly impacts the level of induction.
Understanding this concept is crucial, as it forms the basis of alternating current generation and helps ensure that the generator is correctly designed to meet required specifications.
Rotational Motion
Rotational motion is pivotal in the functioning of AC generators. It's the motion of an object in a circular path around a central point or axis. For a generator, this involves the rotation of a coil in a magnetic field to produce electricity.

In our context, knowing how to compute the necessary speed of rotation to achieve an output of 120 V is essential. The angular velocity, denoted as \( \omega \), plays a key role here as it determines how fast the coil turns within the magnetic field. The formula \( \varepsilon_{max} = NAB \omega \) relates these quantities. By rearranging, we can solve for \( \omega \) and determine the ideal rotation speed.

Key points about rotational motion include:
  • Angular velocity measures how fast an object is rotating and is usually expressed in radians per second (rad/s).
  • Converting between different units such as rad/s to revolutions per minute (rpm) is often necessary to match practical applications.
This understanding enables us to design the generator to function at optimal rotation speeds.
Coil Resistance
Coil resistance is an important factor when designing or analyzing an AC generator. It refers to the opposition to the flow of current through the coil due to its material, length, thickness, and temperature.

In the exercise, you must ensure the coil has an "acceptable" resistance, which influences efficiency and performance. High resistance can lead to power loss in the form of heat and reduce the generator’s efficiency.

Factors influencing coil resistance include:
  • The number of loops or turns in the coil: More turns can mean more resistance due to longer wire length.
  • The material of the wire: Conductive materials like copper are preferred due to their low resistivity.
Balancing resistance with other design aspects like coil size and number of loops ensures the generated voltage meets the target specifications without unnecessary energy loss.

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Most popular questions from this chapter

CALC In a region of space, a magnetic field points in the \(+x\) -direction (toward the right). Its magnitude varies with position according to the formula \(B_{x}=B_{0}+b x,\) where \(B_{0}\) and \(b\) are positive constants, for \(x \geq 0 .\) A flat coil of area \(A\) moves with uniform speed \(v\) from right to left with the plane of its area always perpendicular to this field. (a) What is the emf induced in this coil while it is to the right of the origin? (b) As viewed from the origin, what is the direction (clockwise or counterclockwise) of the current induced in the coil? (c) If instead the coil moved from left to right, what would be the answers to parts (a) and (b)?

CALC A conducting rod with length \(L=0.200 \mathrm{m},\) mass \(m=0.120 \mathrm{kg},\) and resistance \(R=80.0 \Omega\) moves without friction on metal rails as shown in Fig. \(29.11 .\) A uniform magnetic field with magnitude \(B=1.50 \mathrm{T}\) is directed into the plane of the figure. The rod is initially at rest, and then a constant force with magnitude \(F=1.90 \mathrm{N}\) and directed to the right is applied to the bar. How many seconds after the force is applied does the bar reach a speed of \(25,0 \mathrm{m} / \mathrm{s} ?\)

CALC A coil 4.00 \(\mathrm{cm}\) in radius, containing 500 turns, is placed in a uniform magnetic field that varies with time according to \(B=(0.0120 \mathrm{T} / \mathrm{s}) t+\left(3.00 \times 10^{-5} \mathrm{T} / \mathrm{s}^{4}\right) t^{4} .\) The coil is connected to a \(600-\Omega\) resistor, and its plane is perpendicular to the magnetic field. You can ignore the resistance of the coil. (a) Find the magnitude of the induced emf in the coil as a function of time. (b) What is the current in the resistor at time \(t=5.00 \mathrm{s?}\)

CALC A dielectric of permittivity \(3.5 \times 10^{-11} \mathrm{F} / \mathrm{m}\) completely fills the volume between two capacitor plates. For \(t>0\) the electric flux through the dielectric is \(\left(8.0 \times 10^{3} \mathrm{V} \cdot \mathrm{s} / \mathrm{s}^{3}\right) t^{3}\) . The dielectric is ideal and nonmagnetic; the conduction current in the dielectric is zero. At what time does the displacement current in the dielectric equal 21\(\mu \mathrm{A} ?\)

The magnetic field within a long, straight solenoid with a circular cross section and radius \(R\) is increasing at a rate of \(d B / d t\) . (a) What is the rate of change of flux through a circle with radius \(r_{1}\) inside the solenoid, normal to the axis of the solenoid, and with center on the solenoid axis? (b) Find the magnitude of the induced electric field inside the solenoid, at a distance \(r_{1}\) from its axis. Show the direction of this field in a diagram. (c) What is the magnitude of the induced electric field outside the solenoid, at a distance \(r_{2}\).from the axis? (d) Graph the magnitude of the induced electric field as a function of the distance \(r\) from the axis from \(r=0\) to \(r=2 R\) (e) What is the magnitude of the induced emf in a circular turn of radius \(R / 2\) that has its center on the solenoid axis? (f) What is the magnitude of the induced emf if the radius in part (e) is \(R ?\) (g) What is the induced emf if the radius in part (e) is 2R?

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