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?
You are standing a distance x = 1.75 m away from this mirror. The object you are looking at is y = 0.29 m from the mirror. The angle of incidence is θ = 30°. What is the exact distance from you to the image?
For each of the actions depicted below, a magnet and/or metal loop moves with velocity v→ (v→ is constant and has the same magnitude in all parts). Determine whether a current is induced in the metal loop. If so, indicate the direction of the current in the loop, either clockwise or counterclockwise when seen from the right of the loop. The axis of the magnet is lined up with the center of the loop. For the action depicted in (Figure 5), indicate the direction of the induced current in the loop (clockwise, counterclockwise or zero, when seen from the right of the loop). I know that the current is clockwise, I just dont understand why. Please fully explain why it's clockwise, Thank you
A planar double pendulum consists of two point masses \[m_1 = 1.00~\mathrm{kg}, \qquad m_2 = 1.00~\mathrm{kg}\]connected by massless, rigid rods of lengths \[L_1 = 1.00~\mathrm{m}, \qquad L_2 = 1.20~\mathrm{m}.\]The upper rod is hinged to a fixed pivot; gravity acts vertically downward with\[g = 9.81~\mathrm{m\,s^{-2}}.\]Define the generalized coordinates \(\theta_1,\theta_2\) as the angles each rod makes with thedownward vertical (positive anticlockwise, measured in radians unless stated otherwise).At \(t=0\) the system is released from rest with \[\theta_1(0)=120^{\circ}, \qquad\theta_2(0)=-10^{\circ}, \qquad\dot{\theta}_1(0)=\dot{\theta}_2(0)=0 .\]Using the exact nonlinear equations of motion (no small-angle or planar-pendulumapproximations) and assuming the rods never stretch or slip, determine the angle\(\theta_2\) at the instant\[t = 10.0~\mathrm{s}.\]Give the result in degrees, in the interval \((-180^{\circ},180^{\circ}]\).
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