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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.

Short Answer

Expert verified
Answer: The potential difference induced between the man's head and feet is 18.0 V.

Step by step solution

01

Identify the given values

We are given the following values in the problem: - Height of the man (L): 1.80 m - Walking speed (v): 2.00 m/s - Magnetic field (B): 5.0 T
02

Apply the motional EMF formula

Using the given values, we can apply the motional EMF formula to find the potential difference induced in the man's body. As we mentioned earlier, the formula is: EMF = vBL Plugging in the given values, we get: EMF = (2.00 m/s)(5.0 T)(1.80 m)
03

Calculate the potential difference

Now, we will multiply the values together to find the potential difference: EMF = 18.0 V The potential difference induced between the man's head and feet is 18.0 V.

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Key Concepts

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

Magnetic Fields
Magnetic fields are fundamental forces of nature, often visualized as lines of force that exit a magnetic north pole and enter a magnetic south pole. These fields are created by moving charges, such as an electric current flowing through a wire, or by the intrinsic magnetic moments of elementary particles associated with a fundamental quantum property called spin.

Magnetic fields exert forces on other moving charges or magnetic materials within the field. This interaction is the basis for the operation of countless devices, from electric motors to MRI machines. In our exercise, a strong magnetic field of 5.0 Tesla, which is far greater than the Earth's natural magnetic field, interacts with the conducting elements inside the human body, leading to an induced potential difference.
Electromagnetic Induction
Electromagnetic induction is a process where a conductor moving through a magnetic field, or a changing magnetic field around a stationary conductor, induces an electromotive force (EMF), or voltage. This phenomenon was discovered by Michael Faraday and is harnessed in many electrical devices such as generators and transformers.

In the textbook exercise, as the man walks perpendicularly through a magnetic field, his body acts as a conductor and experiences this fundamental effect. The fluids in his body containing charged particles (ions) move through the magnetic field, which induces an EMF along the length of his body, creating a potential difference between his head and feet. This potential difference can be calculated using the formula EMF = vBL, where 'v' is the velocity of the conductor, 'B' is the magnetic field strength, and 'L' is the length of the conductor.
Electric Fields
Electric fields represent the force fields surrounding electric charges, and they exert forces on other charges within the field. The strength of the electric field at each point is defined as the force per unit charge that would be felt by a stationary test charge placed at that point. These fields are crucial to understanding the behavior of charges and the flow of current in conductive materials.

Although our exercise focuses primarily on the effects of a magnetic field, the concept of electric fields is inherently linked due to the induced EMF. The generated potential difference within the man's body implies the existence of an electric field directed along his body's length. If left unhindered, this electric field would cause current to flow within the body. Fortunately, the human body has high resistance which prevents dangerous currents from flowing in such situations.

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Most popular questions from this chapter

You have a light bulb, a bar magnet, a spool of wire that you can cut into as many pieces as you want, and nothing else. How can you get the bulb to light up? a) You can't. The bulb needs electricity to light it, not magnetism. b) You cut a length of wire, connect the light bulb to the two ends of the wire, and pass the magnet through the loop that is formed. c) You cut two lengths of wire and connect the magnet and the bulb in series.

A metal loop has an area of \(0.100 \mathrm{~m}^{2}\) and is placed flat on the ground. There is a uniform magnetic field pointing due west, as shown in the figure. This magnetic field initially has a magnitude of \(0.123 \mathrm{~T}\), which decreases steadily to \(0.075 \mathrm{~T}\) during a period of \(0.579 \mathrm{~s}\). Find the potential difference induced in the loop during this time.

A short coil with radius \(R=10.0 \mathrm{~cm}\) contains \(N=30.0\) turns and surrounds a long solenoid with radius \(r=8.00 \mathrm{~cm}\) containing \(n=60\) turns per centimeter. The current in the short coil is increased at a constant rate from zero to \(i=2.00 \mathrm{~A}\) in a time of \(t=12.0 \mathrm{~s}\). Calculate the induced potential difference in the long solenoid while the current is increasing in the short coil.

A popular demonstration of eddy currents involves dropping a magnet down a long metal tube and a long glass or plastic tube. As the magnet falls through a tube, there is changing flux as the magnet falls toward or away from each part of the tube. a) Which tube has the larger voltage induced in it? b) Which tube has the larger eddy currents induced in it?

An ideal battery (with no internal resistance) supplies \(V_{\mathrm{emf}}\) and is connected to a superconducting (no resistance!) coil of inductance \(L\) at time \(t=0 .\) Find the current in the coil as a function of time, \(i(t) .\) Assume that all connections also have zero resistance.

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