You are standing at a spot where the magnetic field of the Earth is horizontal, points due northward, and has magnitude \(40.0 \mu \mathrm{T}\). Directly above your head, at a height of \(12.0 \mathrm{~m},\) a long, horizontal cable carries a steady \(\mathrm{DC}\) current of 500.0 A due northward. Calculate the angle \(\theta\) by which your magnetic compass needle is deflected from true magnetic north by the effect of the cable. Don't forget the sign of \(\theta-\) is the deflection eastward or westward?

Short Answer

Expert verified
Given: Magnetic field of the Earth: \(40.0 \, \mu T\) Height of the cable above the ground: \(12.0 \, m\) Current carried by the cable: \(500.0 A\) Following the steps outlined in the solution, carry out the calculations and find the angle of deflection, which is: \(\theta = -22.7°\) The compass needle is deflected by an angle of \(-22.7°\) westward from the true magnetic north due to the effect of the horizontal cable carrying the steady DC current.

Step by step solution

01

Calculate the magnetic field due to the wire

First, we need to calculate the magnetic field (\(B_{wire}\)) produced by the wire at the position of the person using the formula for the magnetic field produced by a long straight current-carrying wire. The formula is given by: \(B_{wire} = \frac{\mu_0 I}{2\pi d}\) Where \(B_{wire}\) is the magnetic field produced by the wire, \(\mu_0\) is the permeability of free space (\(4\pi \times 10^{-7} \, Tm/A\)), \(I\) is the current in the wire (500.0 A), and \(d\) is the distance from the wire to the person (12.0 m). Now, let's plug in the values and calculate the magnetic field due to the wire. \(B_{wire} = \frac{4\pi \times 10^{-7} \, Tm/A * 500.0 \, A}{2\pi * 12.0 \, m} = 1.67 \times 10^{-5} \, T\)
02

Find the net magnetic field

Next, let's find the net magnetic field (\(B_{net}\)) by adding the Earth's magnetic field (\(B_{earth}\)) which is given as \(40.0 \, \mu T\) (horizontal and northward) and the magnetic field due to the wire (\(B_{wire}\)), which is horizontal and points westward. Since the Earth's magnetic field and the magnetic field due to the wire are perpendicular to each other, we can use the Pythagorean theorem to find the magnitude of the net magnetic field. \(B_{net} = \sqrt{B_{earth}^2 + B_{wire}^2} = \sqrt{(40.0 \times 10^{-6}\, T)^2 + (1.67 \times 10^{-5}\, T)^2} = 4.32 \times 10^{-5} \, T\)
03

Calculate the angle of deflection

Now that we have the net magnetic field, we can find the angle \(\theta\) of deflection by considering the ratio of the magnetic field due to the wire (\(B_{wire}\)) and the Earth's magnetic field (\(B_{earth}\)). We can use the tangent function and calculate the angle as follows: \(\tan{\theta} = \frac{B_{wire}}{B_{earth}}\) \(\theta = \arctan{\frac{B_{wire}}{B_{earth}}} = \arctan{\frac{1.67 \times 10^{-5}\, T}{40.0 \times 10^{-6} \, T}} = 22.7°\) Since the magnetic field due to the wire points westward, the compass needle is deflected by \(22.7°\) westward (which is negative in this context). So, \(\theta = -22.7°\).

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