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A respiration monitor has a flexible loop of copper wire, which wraps about the chest. As the wearer breathes, the radius of the loop of wire increases and decreases. When a person in the Earth's magnetic field (assume \(0.426 \cdot 10^{-4} \mathrm{~T}\) ) inhales, what is the average current in the loop, assuming that it has a resistance of \(30.0 \Omega\) and increases in radius from \(20.0 \mathrm{~cm}\) to \(25.0 \mathrm{~cm}\) over 1.00 s? Assume that the magnetic field is perpendicular to the plane of the loop.

Short Answer

Expert verified
Using Faraday's Law of electromagnetic induction, we find the average current in a flexible loop of copper wire as the wearer inhales by following these steps: 1. Calculate the change in magnetic flux: \(\Delta \Phi = (0.426 \cdot 10^{-4} \mathrm{~T}) (\pi (25.0 \mathrm{~cm})^2 - \pi (20.0 \mathrm{~cm})^2)\) 2. Calculate the induced EMF: \(\epsilon = -\frac{\Delta \Phi}{1.00 \mathrm{~s}}\) 3. Calculate the average current: \(I = \frac{\epsilon}{30.0 \Omega}\) The average current is found to be \(2.81 \times 10^{-6} A\), or \(2.81 \mathrm{~\mu A}\).

Step by step solution

01

Calculate the change in magnetic flux

To find the induced EMF, we first need to calculate the change in magnetic flux through the loop. The magnetic flux \(\Phi\) through a loop is given by: \(\Phi = B \cdot A \cdot \cos{\theta}\) where \(B\) is the magnetic field, \(A\) is the area of the loop, and \(\theta\) is the angle between the magnetic field and the normal to the loop's plane. In our case, the magnetic field is perpendicular to the plane of the loop, so \(\theta = 90^\circ\) and \(\cos{\theta} = 1\). The area of the loop is the area of a circle, which is given by: \(A = \pi r^2\) where \(r\) is the radius of the loop. The change in magnetic flux is therefore: \(\Delta \Phi = \Phi_{final} - \Phi_{initial} = B \cdot (A_{final}-A_{initial})\)
02

Calculate the induced EMF

Now that we have the change in magnetic flux, we can use Faraday's Law to find the induced EMF: \(\epsilon = -\frac{\Delta \Phi}{\Delta t}\) where \(\epsilon\) is the induced EMF and \(\Delta t\) is the change in time.
03

Calculate the average current

Finally, we can use Ohm's Law to find the average current in the loop: \(I = \frac{\epsilon}{R}\) where \(I\) is the average current and \(R\) is the resistance of the loop. We can substitute the known values to find the average current.
04

Step 1

Calculate the change in magnetic flux: \(\Delta \Phi = (0.426 \cdot 10^{-4} \mathrm{~T}) (\pi (25.0 \mathrm{~cm})^2 - \pi (20.0 \mathrm{~cm})^2)\).
05

Step 2

Calculate the induced EMF: \(\epsilon = -\frac{\Delta \Phi}{1.00 \mathrm{~s}}\).
06

Step 3

Calculate the average current: \(I = \frac{\epsilon}{30.0 \Omega}\). After plugging in the values from the previous steps and performing the calculations, we find the average current to be \(2.81 \times 10^{-6} A\), or \(2.81 \mathrm{~\mu A}\).

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Most popular questions from this chapter

Faraday's Law of Induction states that a) a potential difference is induced in a loop when there is a change in the magnetic flux through the loop. b) the current induced in a loop by a changing magnetic field produces a magnetic field that opposes this change in magnetic field. c) a changing magnetic field induces an electric field. d) the inductance of a device is a measure of its opposition to changes in current flowing through it. e) magnetic flux is the product of the average magnetic field and the area perpendicular to it that it penetrates.

A student wearing a \(15.0-\mathrm{g}\) gold band with radius \(0.750 \mathrm{~cm}\) (and with a resistance of \(61.9 \mu \Omega\) and a specific heat capacity of \(c=129 \mathrm{~J} / \mathrm{kg}^{\circ} \mathrm{C}\) ) on her finger moves her finger from a region having a magnetic field of \(0.0800 \mathrm{~T}\) pointing along her finger, to a region with zero magnetic field in \(40.0 \mathrm{~ms}\). As a result of this action, thermal energy is added to the band due to the induced current, which raises the temperature of the band. Calculate the temperature rise in the band, assuming that all the energy produced is used in raising the temperature.

Large electric fields are certainly a hazard to the human body, as they can produce dangerous currents, but what about large magnetic fields? A man \(1.80 \mathrm{~m}\) tall walks at \(2.00 \mathrm{~m} / \mathrm{s}\) perpendicular to a horizontal magnetic field of \(5.0 \mathrm{~T}\); that is, he walks between the pole faces of a very big magnet. (Such a magnet can, for example, be found in the National Superconducting Cyclotron Laboratory at Michigan State University.) Given that his body is full of conducting fluids, estimate the potential difference induced between his head and feet.

A wedding ring (of diameter \(1.95 \mathrm{~cm}\) ) is tossed into the air and given a spin, resulting in an angular velocity of 13.3 rev/s. The rotation axis is a diameter of the ring. If the magnitude of the Earth's magnetic field at the ring's location is \(4.77 \cdot 10^{-5} \mathrm{~T}\), what is the maximum induced potential difference in the ring?

What is the inductance in a series \(\mathrm{RL}\) circuit in which \(R=3.00 \mathrm{k} \Omega\) if the current increases to \(\frac{1}{2}\) of its final value in \(20.0 \mu \mathrm{s} ?\)

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