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Ch 27: Magnetic Field and Magnetic Forces
Chapter 27, Problem 27

A deuteron (the nucleus of an isotope of hydrogen) has a mass of 3.34x10^-27 kg and a charge of +e. The deuteron travels in a circular path with a radius of 6.96 mm in a magnetic field with magnitude 2.50 T. (a) Find the speed of the deuteron. (b) Find the time required for it to make half a revolution. (c) Through what potential difference would the deuteron have to be accelerated to acquire this speed?

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Step 1: Use the formula for the magnetic force acting on a moving charge, which is given by \( F = qvB \), where \( F \) is the magnetic force, \( q \) is the charge, \( v \) is the velocity, and \( B \) is the magnetic field strength. Since the deuteron moves in a circular path, the magnetic force provides the necessary centripetal force, \( F_c = \frac{mv^2}{r} \), where \( m \) is the mass of the deuteron and \( r \) is the radius of the circular path.
Step 2: Equate the magnetic force to the centripetal force to find the velocity of the deuteron. Solve the equation \( qvB = \frac{mv^2}{r} \) for \( v \).
Step 3: Calculate the time required for half a revolution. The circumference of the full circular path is \( 2\pi r \). The time for one full revolution is the period \( T \), given by \( T = \frac{2\pi r}{v} \). For half a revolution, the time is \( \frac{T}{2} \).
Step 4: To find the potential difference needed to accelerate the deuteron to this speed, use the kinetic energy formula \( K = \frac{1}{2} mv^2 \). The kinetic energy acquired by the deuteron comes from the electric potential energy, which is \( qV \), where \( V \) is the potential difference. Therefore, set \( \frac{1}{2} mv^2 = qV \) and solve for \( V \).
Step 5: Substitute the values of \( m \), \( q \), \( r \), and \( B \) into the equations derived in the previous steps to calculate the numerical values for the speed, time for half a revolution, and the required potential difference.

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Key Concepts

Here are the essential concepts you must grasp in order to answer the question correctly.

Lorentz Force

The Lorentz force is the force experienced by a charged particle moving through a magnetic field. It is given by the equation F = q(v × B), where F is the force, q is the charge, v is the velocity of the particle, and B is the magnetic field. This force is responsible for the circular motion of the deuteron in the magnetic field, as it acts perpendicular to the velocity, causing centripetal acceleration.
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Centripetal Force

Centripetal force is the net force that acts on an object moving in a circular path, directed towards the center of the circle. For a charged particle like the deuteron in a magnetic field, the magnetic force acts as the centripetal force, allowing us to relate the particle's mass, speed, and radius of the circular path through the equation F_c = (mv^2)/r, where m is mass, v is speed, and r is radius.
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Kinetic Energy and Potential Difference

The kinetic energy of a charged particle is given by KE = (1/2)mv^2, where m is mass and v is speed. When a charged particle is accelerated through a potential difference (V), it gains kinetic energy equal to the work done on it, expressed as KE = qV, where q is the charge. This relationship allows us to calculate the potential difference required to accelerate the deuteron to a specific speed.
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Related Practice
Textbook Question
A straight, 2.5-m wire carries a typical household current of 1.5 A (in one direction) at a location where the earth's magnetic field is 0.55 gauss from south to north. Find the magnitude and direction of the force that our planet's magnetic field exerts on this wire if it is oriented so that the current in it is running (a) from west to east, (b) vertically upward, (c) from north to south. (d) Is the magnetic force ever large enough to cause significant effects under normal household conditions?

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Textbook Question
Cyclotrons are widely used in nuclear medicine for producing short-lived radioactive isotopes. These cyclotrons typically accelerate H- (the hydride ion, which has one proton and two electrons) to an energy of 5 MeV to 20 MeV. This ion has a mass very close to that of a proton because the electron mass is negligible—about 1/2000 of the proton's mass. A typical magnetic field in such cyclotrons is 1.9 T. (a) What is the speed of a 5.0-MeV H-? (b) If the H- has energy 5.0 MeV and B = 1.9 T, what is the radius of this ion's circular orbit?
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Textbook Question
In a cyclotron, the orbital radius of protons with energy 300 keV is 16.0 cm. You are redesigning the cyclotron to be used instead for alpha particles with energy 300 keV. An alpha particle has charge q = +2e and mass m = 6.64x10^-27 kg. If the magnetic field isn't changed, what will be the orbital radius of the alpha particles?
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Textbook Question
A beam of protons traveling at 1.20 km/s enters a uniform magnetic field, traveling perpendicular to the field. The beam exits the magnetic field, leaving the field in a direction perpendicular to its original direction (Fig. E27.24) . The beam travels a distance of 1.18 cm while in the field. What is the magnitude of the magnetic field?
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Textbook Question
A long wire carrying 4.50 A of current makes two 90° bends, as shown in Fig. E27.35

. The bent part of the wire passes through a uniform 0.240-T magnetic field directed as shown in the figure and confined to a limited region of space. Find the magnitude and direction of the force that the magnetic field exerts on the wire.
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