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A coil consists of \(120 .\) circular loops of wire of radius \(4.80 \mathrm{~cm} .\) A current of 0.490 A runs through the coil, which is oriented vertically and is free to rotate about a vertical axis (parallel to the \(z\) -axis). It experiences a uniform horizontal magnetic field in the positive \(x\) -direction. When the coil is oriented parallel to the \(x\) -axis, a force of \(1.20 \mathrm{~N}\) applied to the edge of the coil in the positive \(y\) -direction can keep it from rotating. Calculate the strength of the magnetic field.

Short Answer

Expert verified
Answer: The strength of the magnetic field is approximately \(7.13 \times 10^{-3}\,\text{T}\).

Step by step solution

01

Calculate the magnetic force on the coil due to the magnetic field

To find the strength of the magnetic field, we'll need the magnetic force acting on the coil due to the magnetic field. The formula for the magnetic force on a current-carrying loop is given by: \(F_B = N \cdot I \cdot A \cdot B \cdot sin \theta\) Where: F_B = magnetic force on the coil N = number of loops in the coil (120 loops) I = current in the coil (0.490A) A = area of each loop (\(pi r^2\), with r = 0.048m) B = strength of the magnetic field sinθ = sine of the angle between the normal to the plane of the coil and the direction of the magnetic field (1 for parallel orientation)
02

Calculate the torque on the coil due to the applied force

The next step is to determine the torque on the coil due to the applied force. We can calculate the torque using the formula: \(τ = F \cdot d\) Where: τ = torque F = applied force (1.20 N) d = distance from the axis of rotation to the point where the force is applied (radius of the coil, 0.048m)
03

Calculate the torque on the coil due to the magnetic field

Since the coil is not rotating, the torque due to the applied force is equal to the torque due to the magnetic force. We can calculate the torque due to the magnetic force using the formula: \(τ = N \cdot I \cdot A \cdot B \cdot r\) Where: τ = torque N, I, A, and r are the same as from Step 1 B = strength of the magnetic field
04

Find the strength of the magnetic field

Now that we have the torque due to the applied force and the magnetic force, we can equate them to find the strength of the magnetic field: \(1.20\cdot0.048 = 120 \cdot 0.490 \cdot (\pi\cdot0.048^2) \cdot B\) Solving for B, we get: \(B = \frac{1.20\cdot0.048}{120 \cdot 0.490 \cdot (\pi\cdot0.048^2)}\) Calculating the value of B: \(B \approx 7.13 \times 10^{-3}\,\text{T}\) Hence, the strength of the magnetic field is approximately \(7.13 \times 10^{-3}\,\text{T}\).

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Most popular questions from this chapter

A velocity selector is used in a mass spectrometer to produce a beam of charged particles of uniform velocity. Suppose the fields in a selector are given by \(\vec{E}=E_{x} \hat{x}\) and \(\vec{B}=(47.45 \mathrm{mT}) \hat{y} .\) The speed with which a charged particle can travel through the selector in the \(z\) -direction without being deflected is \(5.616 \cdot 10^{5} \mathrm{~m} / \mathrm{s}\). What is the value of \(E_{x} ?\)

A particle with a charge of \(+10.0 \mu \mathrm{C}\) is moving at \(300 \mathrm{~m} / \mathrm{s}\) in the positive \(z\) -direction. a) Find the minimum magnetic field required to keep it moving in a straight line at constant speed if there is a uniform electric field of magnitude \(100 . \mathrm{V} / \mathrm{m}\) pointing in the positive \(y\) -direction. b) Find the minimum magnetic field required to keep the particle moving in a straight line at constant speed if there is a uniform electric field of magnitude \(100 . \mathrm{V} / \mathrm{m}\) pointing in the positive \(z\) -direction.

A \(12.0-\mathrm{V}\) battery is connected to a \(3.00-\Omega\) resistor in a rigid rectangular loop of wire measuring \(3.00 \mathrm{~m}\) by \(1.00 \mathrm{~m}\). As shown in the figure, a length \(\ell=1.00 \mathrm{~m}\) of wire at the end of the loop extends into a \(2.00 \mathrm{~m}\) by \(2.00 \mathrm{~m}\) region with a magnetic field of magnitude \(5.00 \mathrm{~T}\) directed into the page. What is the net force on the loop?

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A cyclotron in a magnetic field of \(9.00 \mathrm{~T}\) is used to accelerate protons to \(50.0 \%\) of the speed of light. What is the cyclotron frequency of these protons? What is the radius of their trajectory in the cyclotron? What are the cyclotron frequency and the trajectory radius of the same protons in the Earth's magnetic field? Assume that the Earth's magnetic field is 0.500 G.

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