Show that the magnitude of the magnetic field B along the positive z-axis through the center of a circular loop that carries a steady current I (see Fig. 1) can be expressed as HOIR²N 2(R² + z²)3/2 where R is the radius of the loop and N is the number of turns in the current loop. B(z) =

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Chapter24: Magnetic Fields
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Problem 102A
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Part 2: Dual Coil Experiment:
In the following experiment, you will measure the spatial dependence of the magnetic field along the
z-axis above a multi-turn coil. Rather than using a constant (DC) current source that would produce
a static magnetic field, you will use a time-varying, alternating current (AC) source that will produce
a time-varying magnetic field. The time-varying magnetic field will produce a time-varying magnetic
flux through a pick-up coil, and you will measure the resulting induced emf (in volts).
2.1 Show that the magnitude of the magnetic field B along the positive z-axis through the center of a
circular loop that carries a steady current I (see Fig. 1) can be expressed as
HOIR²N
2(R² + z²)³/2
where R is the radius of the loop and N is the number of turns in the current loop.
B(z)
R
=
Z
2
I
(5)
Figure 1: A circular loop of wire, with N turns, carrying a current I. The magnetic field is given along the
positive z-axis.
Transcribed Image Text:Part 2: Dual Coil Experiment: In the following experiment, you will measure the spatial dependence of the magnetic field along the z-axis above a multi-turn coil. Rather than using a constant (DC) current source that would produce a static magnetic field, you will use a time-varying, alternating current (AC) source that will produce a time-varying magnetic field. The time-varying magnetic field will produce a time-varying magnetic flux through a pick-up coil, and you will measure the resulting induced emf (in volts). 2.1 Show that the magnitude of the magnetic field B along the positive z-axis through the center of a circular loop that carries a steady current I (see Fig. 1) can be expressed as HOIR²N 2(R² + z²)³/2 where R is the radius of the loop and N is the number of turns in the current loop. B(z) R = Z 2 I (5) Figure 1: A circular loop of wire, with N turns, carrying a current I. The magnetic field is given along the positive z-axis.
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