In magnetic resonance imaging (MRI), a patient lies in a strong
1- to 2-TT magnetic field B⃗ B→ oriented parallel to the body. This
field is produced by a large superconducting solenoid. The MRI
measurements depend on the magnetic dipole moment μ⃗ μ→ of a
proton, the nucleus of a hydrogen atom. The proton magnetic dipoles
can have only two orientations: either with the field or against
the field. The energy needed to reverse this orientation ("flip"
the protons) from with the field to against the field is exactly
ΔU=2μBΔU=2μB (like the energy needed to turn a compass needle from
north to south).
The pulse of a radio frequency probe field irradiates the patient's
body in the region to be imaged. If this probe field is tuned
correctly so that its energy equals the ΔU=2μBΔU=2μB needed to
reverse the orientation of the protons from with the external BB
field to against it, a reasonable number of protons will flip. When
the protons return to their initial orientation and a lower energy
state, they emit this same radio frequency radiation in different
directions. This radiation is detected and provides a measure of
the concentration of protons in the region irradiated by the probe
field. The proton concentration differs in fat, muscle, and bone
tissue, and in healthy and diseased tissue. Thus, the probe signal
makes an image of the tissue type in each local region.
The MRI image of an internal body part is made by adjusting an
auxiliary magnetic field, which varies the external BB field over
the region being examined so that the probe field energy equals the
flipping energy ΔU=2μBΔU=2μB in only a small area of the body. A
measurement is made at that point. The external magnetic field is
then adjusted to flip protons in a neighboring small area of the
body. Continual shifts in the magnetic field and detection of
proton concentrations at different tiny locations produce a map of
proton concentration in the body. The MRI image of the lower back
in the figure indicates an L45 disk that has partially collapsed-it
has lost water and because it contains fewer protons produces a
darker MRI image.
The energy of the probe field causes protons to flip when in a 1.50-TT magnetic field. A ±± 1.30×10−3-TT variation in the magnetic field causes a mismatch with the radio frequency flipping field and no flipping at a distance of 2.30×10−3 mm from where the magnetic field is matched to the flipping field. Determine the change in the BB field per unit distance.
Express your answer in teslas per meter.
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