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A closely wound rectangular coil of 80 turns has dimensions of 25.0 \(\mathrm{cm}\) by 40.0 \(\mathrm{cm}\) . The coll is rotated from a position where it makes an angle of \(37.0^{\circ}\) with a magnetic field of 1.10 \(\mathrm{T}\) to a position perpendicular to the field. The rotation takes 0.0600 s. What is the average emf induced in the coil?

Short Answer

Expert verified
117.12 V

Step by step solution

01

Understanding the Problem

We have a rectangular coil with 80 turns, measuring 25.0 cm by 40.0 cm, placed in a magnetic field of 1.10 T. Initially, the coil is at a 37.0° angle to the magnetic field before it is rotated to a perpendicular position (90°). We need to find the average electromotive force (emf) induced as the coil rotates within 0.0600 seconds.
02

Calculation of Coil Area

Calculate the area of the coil, which is the product of its dimensions:\[A = ext{length} imes ext{width} = 25.0 ext{ cm} imes 40.0 ext{ cm} = 1000 ext{ cm}^2 = 0.1 ext{ m}^2\] (Converting cm to m by dividing by 100).
03

Magnetic Flux Initial and Final State

The magnetic flux through the coil is calculated as:\[\Phi = B \cdot A \cdot \cos(\theta)\]Initially, \(\theta = 37.0^{\circ}\):\[\Phi_i = 1.10 \times 0.1 \times \cos(37.0^{\circ}) = 1.10 \times 0.1 \times 0.7986 = 0.08784 \text{ Wb}\]Finally, \(\theta = 90^{\circ}\):\[\Phi_f = 1.10 \times 0.1 \times \cos(90^{\circ}) = 0 \text{ Wb}\]
04

Calculate the Change in Magnetic Flux

The change in magnetic flux (\(\Delta \Phi\)) is given by:\[\Delta \Phi = \Phi_f - \Phi_i = 0 - 0.08784 = -0.08784 \text{ Wb}\]
05

Calculate Average Induced EMF

Using Faraday's Law of Induction, the magnitude of the average induced emf is:\[\text{emf} = -N \cdot \frac{\Delta \Phi}{\Delta t}\]where \(N = 80\) is the number of turns, and \(\Delta t = 0.0600 \text{ s}\):\[\text{emf} = -80 \cdot \frac{-0.08784}{0.0600} = 117.12 \, \text{V}\]
06

Conclusion

The negative sign in Faraday's Law indicates the direction of the induced emf (Lenz's law), which we interpret as the magnitude of the emf being 117.12 V. Therefore, the average emf induced in the coil is \(117.12 \, \text{V}\).

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Key Concepts

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

Electromotive Force (emf)
The electromotive force, often abbreviated as emf, is a crucial concept in the world of electromagnetism. It represents the driving force that causes electrons to move through a circuit, creating an electric current. In the context of Faraday's Law of Induction, emf is generated when there is a change in the magnetic flux passing through a coil. This happens because altering the magnetic field around a coil induces a current. It is essential to note that emf is not a force like gravity, but rather a potential difference generated by the change in magnetic flux.
The concept of emf can be likened to the pressure in a water system, which causes water to flow. In electrical terms, this 'pressure' or potential difference causes charges to move, forming an electric current. While emf is measured in volts, it’s a result of the interaction between a magnetic field and a current-carrying wire. Through Faraday’s Law, we understand that the magnitude of the emf is directly proportional to the rate of change of magnetic flux.
Magnetic Flux
Magnetic flux is a measure of the total magnetic field passing through a given area. It is represented by the symbol Φ and is expressed in Weber (Wb). The magnetic flux through a surface is dependent on the strength of the magnetic field, the area of the surface it penetrates, and the angle at which the field lines pass through the surface. Mathematically, it is given by the equation:
  • \[\Phi = B \cdot A \cdot \cos(\theta)\]
where \(B\) is the magnetic field strength, \(A\) is the area perpendicular to the field lines, and \(\theta\) is the angle between the field lines and the normal to the surface.
A good way to visualize magnetic flux is to imagine a magnetic field passing through a window. As the window rotates or the magnetic field's strength changes, the amount of field "flowing" through the window changes too, altering the magnetic flux. Understanding this concept is key to analyzing how emf is induced in electrical circuits.
Lenz's Law
Lenz's Law is an extension of Faraday's Law, providing a crucial insight into the direction of induced emf and current. It states that the induced emf creates a current that opposes the change in magnetic flux that produced it. This negative feedback loop is essential to the conservation of energy in electromagnetism. Mathematically, Lenz's Law is encapsulated within Faraday's Law of Induction, where the negative sign in the formula \[\text{emf} = -N \cdot \frac{\Delta \Phi}{\Delta t}\], indicates this opposition.
  • Remember, the direction of the induced emf will always counteract the change in the magnetic environment to "resist" its cause.
A helpful analogy is imagining a thermostat that turns on to cool a room down as soon as it starts getting warmer. This opposing action helps to maintain stability and reflects the natural resistance in electrical systems to changes in their magnetic environments.
Coil Area Calculation
Calculating the area of a coil is an essential step when dealing with problems related to magnetic flux and emf. For a rectangular coil, the area can be found using the simple formula: \[A = \text{length} \times \text{width}\].
In exercises involving electromagnetic induction, it is often necessary to convert dimensions from centimeters to meters, as standard units in physics calculations are in meters. For example, if a coil measures 25.0 cm by 40.0 cm, its area in square meters is 0.1 m². This calculation is crucial because the coil's area is fundamental in determining the magnetic flux through the coil, which directly influences the induced emf according to Faraday’s Law.
  • Always check to ensure that measurements are in the correct units before performing calculations.
  • The area determines how much of the magnetic field interacts with the coil, thus affecting the magnitude of the induced emf.

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Most popular questions from this chapter

Motional emfs in Transportation. Airplanes and trains move through the earth's magnetic field at rather high speeds, so it is reasonable to wonder whether this field can have a substantial effect on them. We shall use a typical value of 0.50 G for the earth's field (a) The French TGV train and the Japanese "bullet train" reach speeds of up to 180 mph moving on tracks about 1.5 \(\mathrm{m}\) apart. At top speed moving perpendicular to the earth's magnetic field, what potential difference is induced across the tracks as the wheels roll? Does this seem large enough to produce noticeable effects? (b) The Boeing \(747-400\) aircraft has a wingspan of 64.4 \(\mathrm{m}\) and a cruising speed of 565 mph. If there is no wind blowing (so that this is also their speed relative to the ground), what is the maximum potential difference that could be induced between the opposite tips of the wings? Does this seem large enough to cause problems with the plane?

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 \(t=5.00 \mathrm{s?}\)

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?

Shrinking Loop. A circular loop of flexible iron wire has an initial circumference of 165.0 \(\mathrm{cm} /\) its circumference is decreasing at a constant rate of 12.0 \(\mathrm{cm} / \mathrm{s}\) due to a tangential pull on the wire. The loop is in a constant, uniform magnetic field oriented perpendicular to the plane of the loop and with magnitude 0.500 T. (a) Find the emf induced in the loop at the instant when 9.0 s have passed. (b) Find the direction of the induced current in the loop as viewed looking along the direction of the magnetic field.

A long, straight solenoid with a cross-sectional area of 8.00 \(\mathrm{cm}^{2}\) is wound with 90 turns of wire per centimeter, and the windings carry a current of 0.350 A. A second winding of 12 turns encircles the solenoid at its center. The current in the solenoid is turned off such that the magnetic field of the solenoid becomes zero in 0.0400 s. What is the average induced emf in the second winding?

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