BIO Magnetic fields and MRI . Magnetic resonance imaging (MRI) is a powerful imaging method that, unlike x-ray imaging, can make sharp images of soft tissues without exposing the patient to potentially damaging radiation . A rudimentary understanding of this method can be achieved by the relatively simple application of the classical (that is, non-quantum) physics of magnetism. The starting point for MRI is nuclear magnetic resonance (NMR), a technique that depends on the fact that protons in the atomic nucleus have a magnetic field B → The origin of the proton’s magnetic field is the spin of the proton. Being charged, the spinning proton constitutes an electric current analogous to a wire loop through which current flows. Like the wire loop, the proton has a magnetic moment μ → thus it will experience a torque when it is subjected to an external magnetic field B → 0 The magnitude of μ → is about 1.4 × 10 −26 J/T. The proton can be thought of as being in one of two states, with μ → oriented parallel or antiparallel to the applied magnetic field. Work must be clone to flip the proton from the low-energy state to the high-energy state, as Figure 20.76 shows. Figure 20.76 Problems 86-88. An important consideration is that the ret magnet field of any nucleus, except for that of hydrogen (which has only a proton), consists of contributions from both protons and neutrons. If a nucleus has an even number of protons and neutrons, they pair in such a way that half of the protons have spins in one orientation and half have spins in the other orientation. Thus the net magnetic moment of the nucleus is zero. Only nuclei with a net magnetic moment are candidates for MRI. Hydrogen is the atom that is most commonly imaged. 86. If a proton is exposed to an external magnetic field of 2 T that has a direction perpendicular to the axis of the proton’s spin, what is the torque on the proton? A. 0 B. 1.4 × 10 −26 N · m C. 2.8 × 10 −26 N · m D. 0.7 × 10 −26 N · m
BIO Magnetic fields and MRI . Magnetic resonance imaging (MRI) is a powerful imaging method that, unlike x-ray imaging, can make sharp images of soft tissues without exposing the patient to potentially damaging radiation . A rudimentary understanding of this method can be achieved by the relatively simple application of the classical (that is, non-quantum) physics of magnetism. The starting point for MRI is nuclear magnetic resonance (NMR), a technique that depends on the fact that protons in the atomic nucleus have a magnetic field B → The origin of the proton’s magnetic field is the spin of the proton. Being charged, the spinning proton constitutes an electric current analogous to a wire loop through which current flows. Like the wire loop, the proton has a magnetic moment μ → thus it will experience a torque when it is subjected to an external magnetic field B → 0 The magnitude of μ → is about 1.4 × 10 −26 J/T. The proton can be thought of as being in one of two states, with μ → oriented parallel or antiparallel to the applied magnetic field. Work must be clone to flip the proton from the low-energy state to the high-energy state, as Figure 20.76 shows. Figure 20.76 Problems 86-88. An important consideration is that the ret magnet field of any nucleus, except for that of hydrogen (which has only a proton), consists of contributions from both protons and neutrons. If a nucleus has an even number of protons and neutrons, they pair in such a way that half of the protons have spins in one orientation and half have spins in the other orientation. Thus the net magnetic moment of the nucleus is zero. Only nuclei with a net magnetic moment are candidates for MRI. Hydrogen is the atom that is most commonly imaged. 86. If a proton is exposed to an external magnetic field of 2 T that has a direction perpendicular to the axis of the proton’s spin, what is the torque on the proton? A. 0 B. 1.4 × 10 −26 N · m C. 2.8 × 10 −26 N · m D. 0.7 × 10 −26 N · m
BIO Magnetic fields and MRI. Magnetic resonance imaging (MRI) is a powerful imaging method that, unlike x-ray imaging, can make sharp images of soft tissues without exposing the patient to potentially damaging radiation. A rudimentary understanding of this method can be achieved by the relatively simple application of the classical (that is, non-quantum) physics of magnetism. The starting point for MRI is nuclear magnetic resonance (NMR), a technique that depends on the fact that protons in the atomic nucleus have a magnetic field
B
→
The origin of the proton’s magnetic field is the spin of the proton. Being charged, the spinning proton constitutes an electric current analogous to a wire loop through which current flows. Like the wire loop, the proton has a magnetic moment
μ
→
thus it will experience a torque when it is subjected to an external magnetic field
B
→
0
The magnitude of
μ
→
is about 1.4 × 10−26 J/T. The proton can be thought of as being in one of two states, with
μ
→
oriented parallel or antiparallel to the applied magnetic field. Work must be clone to flip the proton from the low-energy state to the high-energy state, as Figure 20.76 shows.
Figure 20.76
Problems 86-88.
An important consideration is that the ret magnet field of any nucleus, except for that of hydrogen (which has only a proton), consists of contributions from both protons and neutrons. If a nucleus has an even number of protons and neutrons, they pair in such a way that half of the protons have spins in one orientation and half have spins in the other orientation. Thus the net magnetic moment of the nucleus is zero. Only nuclei with a net magnetic moment are candidates for MRI. Hydrogen is the atom that is most commonly imaged.
86. If a proton is exposed to an external magnetic field of 2 T that has a direction perpendicular to the axis of the proton’s spin, what is the torque on the proton?
air is pushed steadily though a forced air pipe at a steady speed of 4.0 m/s. the pipe measures 56 cm by 22 cm. how fast will air move though a narrower portion of the pipe that is also rectangular and measures 32 cm by 22 cm
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13.87 ... Interplanetary Navigation. The most efficient way
to send a spacecraft from the earth to another planet is by using a
Hohmann transfer orbit (Fig. P13.87). If the orbits of the departure
and destination planets are circular, the Hohmann transfer orbit is an
elliptical orbit whose perihelion and aphelion are tangent to the
orbits of the two planets. The rockets are fired briefly at the depar-
ture planet to put the spacecraft into the transfer orbit; the spacecraft
then coasts until it reaches the destination planet. The rockets are
then fired again to put the spacecraft into the same orbit about the
sun as the destination planet. (a) For a flight from earth to Mars, in
what direction must the rockets be fired at the earth and at Mars: in
the direction of motion, or opposite the direction of motion? What
about for a flight from Mars to the earth? (b) How long does a one-
way trip from the the earth to Mars take, between the firings of the
rockets? (c) To reach Mars from the…
Chapter 20 Solutions
College Physics Volume 1 (Chs. 1-16); Mastering Physics with Pearson eText -- ValuePack Access Card -- for College Physics (10th Edition)
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