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An elastic circular conducting loop expands at a constant rate over time such that its radius is given by \(r(t)=r_{0}+v t\), where \(r_{0}=0.100 \mathrm{~m}\) and \(v=0.0150 \mathrm{~m} / \mathrm{s} .\) The loop has a constant resistance of \(R=12.0 \Omega\) and is placed in a uniform magnetic field of magnitude \(B_{0}=0.750 \mathrm{~T}\), perpendicular to the plane of the loop, as shown in the figure. Calculate the direction and the magnitude of the induced current, \(i\), at \(t=5.00 \mathrm{~s}\).

Short Answer

Expert verified
The magnitude of the induced current at t=5s is approximately 0.00103 A, and the direction of the induced current is clockwise within the loop.

Step by step solution

01

Calculate the area of the loop at t=5s

First, we need to find the radius of the loop at t=5s. We can use the given expression for the radius with respect to time: \(r(t)=r_{0}+vt\) \(r(5)=0.100\,\text{m} + 0.0150\,\text{m/s}(5\,\text{s})\) \(r(5)=0.100\,\text{m} + 0.0750\,\text{m} = 0.175\,\text{m}\) Now, we can calculate the area of the loop at t=5s: \(A=\pi r^2\) \(A=\pi (0.175\,\text{m})^2\approx 0.0962\,\text{m}^2\)
02

Calculate the magnetic flux through the loop

To calculate the magnetic flux through the loop, we can use the following expression: \(\Phi = B_{0}\cdot A\) \(\Phi = 0.750\,\text{T} \cdot 0.0962\,\text{m}^2 \approx 0.0722\,\text{Wb}\)
03

Apply Faraday's law of electromagnetic induction

Faraday's law states that the induced electromotive force (EMF) is equal to the negative of the time derivative of the magnetic flux: \(EMF = -\frac{d\Phi}{dt}\) To determine the rate of change of the magnetic flux, we will first need to express the magnetic flux as a function of time: \(\Phi(t) = B_{0} \cdot A(t)\) Now, differentiate the magnetic flux with respect to time: \(\frac{d\Phi(t)}{dt} = B_{0}\frac{dA(t)}{dt}\) To find the rate of change of the area A(t), we need to differentiate the area formula with respect to time: \(A(t) = \pi \cdot r^2(t)\) \(\frac{dA(t)}{dt} = 2\pi\cdot r(t) \cdot \frac{dr(t)}{dt} = 2\pi\cdot r(t)\cdot v\) Now, substituting the given values for r(t) and v: \(\frac{dA(t)}{dt}=2\pi(0.175\,\text{m})(0.0150\,\text{m/s})\approx0.0164\,\text{m}^2/\text{s}\) Now, we can calculate the rate of change of the magnetic flux at t=5s: \(\frac{d\Phi(t)}{dt} = B_{0}\frac{dA(t)}{dt}=0.750\,\text{T}(0.0164\,\text{m}^2/\text{s})\approx0.0123\,\text{Wb/s}\) Finally, we can calculate the induced EMF using Faraday's law: \(EMF = -\frac{d\Phi}{dt} = - 0.0123\,\text{Wb/s}\) The negative sign indicates that the direction of the induced current opposes the change in the magnetic field.
04

Calculate the induced current using Ohm's law

Now that we have the value of the induced EMF, we can calculate the induced current using Ohm's law: \(i = \frac{EMF}{R}\) \(i = \frac{-0.0123\,\text{Wb/s}}{12.0\,\Omega}\approx -0.00103\,\text{A}\)
05

Determine the direction of the induced current

According to Lenz's law, the induced current will flow in such a direction as to oppose the change in the magnetic field. In this case, since the magnetic field is increasing as the loop expands, the induced current will flow in a clockwise direction.
06

Conclusion

The magnitude of the induced current at t=5s is approximately 0.00103 A, and it flows in a clockwise direction within the loop.

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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 is a fundamental principle that describes how a voltage can be induced by changing magnetic environments. The law states that the induced electromotive force (EMF) in any closed circuit is equal to the negative rate of change of the magnetic flux through the circuit. In equation form, it's presented as
\[ EMF = -\frac{d\text{magnetic flux}}{dt} \]

This law is instrumental in understanding how electric generators work and forms the basis of many electrical technologies. Rapid changes in the magnetic field or the movement of a conductor through a static magnetic field can induce this EMF. A negative sign in the equation, known as Lenz's law, signifies that the induced EMF generates a current that opposes the flux change, which is a core concept in electromagnetic induction.
Lenz's Law
Lenz's Law is all about direction – it specifies that the direction of an induced current in a closed conducting loop will always oppose the change in magnetic flux that produced it. Think of it as nature's way of maintaining the status quo. This law complements Faraday's law and is reflected by the negative sign in Faraday's equation.

For instance, if a loop is placed in a magnetic field and the field increases, Lenz's law tells us the induced current will flow in a direction that creates its own magnetic field to counter the increase. If the magnetic field decreases, the induced current's magnetic field will attempt to increase it. This is beautifully illustrated in scenarios where magnets are dropped through conducting tubes and fall more slowly due to the opposing induced currents.
Magnetic Flux
Magnetic flux refers to the measure of the quantity of magnetism, taking into account the strength and the extent of a magnetic field. The formal definition describes it as the total magnetic field which passes through a given area. It's calculated by the equation:

\[ \text{Magnetic flux} (\text{represented by } \text{Φ}) = B \times A \times \text{cos}\theta \]

where \( B \) is the magnetic field strength, \( A \) is the area the field lines pass through, and \( \theta \) is the angle between the magnetic field lines and the normal (perpendicular) to \( A \). Magnetic flux is an essential concept for understanding how the change in flux through a conducting loop relates to the induced EMF and resulting current, as dictated by Faraday's Law.
Ohm's Law
Ohm's Law is a cornerstone of electrical engineering and physics, describing the relationship between voltage, current, and resistance in an electrical circuit. Simply put, this law states that the current through a conductor between two points is directly proportional to the voltage across the two points. It is inversely proportional to the resistance between them. The relationship is summed up with the equation:

\[ I = \frac{V}{R} \]

where \( I \) is the current in amperes, \( V \) is the voltage in volts, and \( R \) is the resistance in ohms. Ohm's Law makes it possible to predict how electric currents will behave in a circuit when subjected to different voltages and resistance levels, thus allowing the design and analysis of electronic components and systems.

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Most popular questions from this chapter

A solid metal disk of radius \(R\) is rotating around its center axis at a constant angular speed of \(\omega .\) The disk is in a uniform magnetic field of magnitude \(B\) that is oriented normal to the surface of the disk. Calculate the magnitude of the potential difference between the center of the disk and the outside edge.

A \(100 .-V\) battery is connected in series with a \(500 .-\Omega\) resistor. According to Faraday's Law of Induction, current can never change instantaneously, so there is always some "stray" inductance. Suppose the stray inductance is \(0.200 \mu \mathrm{H}\). How long will it take the current to build up to within \(0.500 \%\) of its final value of \(0.200 \mathrm{~A}\) after the resistor is con- nected to the battery?

Which of the following statements regarding self induction is correct? a) Self-induction occurs only when a direct current is flowing through a circuit. b) Self-induction occurs only when an alternating current is flowing through a circuit. c) Self-induction occurs when either a direct current or an alternating current is flowing through a circuit. d) Self-induction occurs when either a direct current or an alternating current is flowing through a circuit as long as the current is varying.

A wedding ring (of diameter \(2.0 \mathrm{~cm}\) ) is tossed into the air and given a spin, resulting in an angular velocity of 17 rotations per second. The rotation axis is a diameter of the ring. Taking the magnitude of the Earth's magnetic field to be \(4.0 \cdot 10^{-5} \mathrm{~T}\), what is the maximum induced potential difference in the ring?

A circular conducting loop with radius \(a\) and resistance \(R_{2}\) is concentric with a circular conducting loop with radius \(b \gg a(b\) much greater than \(a\) ) and resistance \(R_{1}\). A time-dependent voltage is applied to the larger loop, having a slow sinusoidal variation in time given by \(V(t)=V_{0} \sin \omega t\) where \(V_{0}\) and \(\omega\) are constants with dimensions of voltage and inverse time, respectively. Assuming that the magnetic field throughout the inner loop is uniform (constant in space) and equal to the field at the center of the loop, derive expressions for the potential difference induced in the inner loop and the current \(i\) through that loop.

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