Imagine two concentric nested infinite solenoids having the same number of turns per unit length, but with radii R and 2R, respectively, and carrying currents I in opposite directions. Calculate the magnetic field a. in the region inside both solenoids, b. in the region between the solenoids (Hint: the answer is |Bvector| = μ0 * I * N / L), and c. in the region outside the solenoids. Assume that the thickness of current-carrying regions are negligible. Note that the magnetic field inside and outside an infinite solenoid with N turns of length L is Bvector = Bz * zhat, where Bz = 0 outside and Bz = μ0 * I * N / L inside its hollow interior.
Imagine two concentric nested infinite solenoids having the same number of turns per unit length, but with radii R and 2R, respectively, and carrying currents I in opposite directions. Calculate the magnetic field a. in the region inside both solenoids, b. in the region between the solenoids (Hint: the answer is |Bvector| = μ0 * I * N / L), and c. in the region outside the solenoids. Assume that the thickness of current-carrying regions are negligible. Note that the magnetic field inside and outside an infinite solenoid with N turns of length L is Bvector = Bz * zhat, where Bz = 0 outside and Bz = μ0 * I * N / L inside its hollow interior.
Chapter12: Sources Of Magnetic Fields
Section: Chapter Questions
Problem 81AP: A long, straight, cylindrical conductor contains a cylindrical cavity whose axis is displaced by n...
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Imagine two concentric nested infinite solenoids having the same number of turns per unit length, but with radii R and 2R, respectively, and carrying currents I in opposite directions. Calculate the magnetic field
a. in the region inside both solenoids,
b. in the region between the solenoids (Hint: the answer is |Bvector| = μ0 * I * N / L), and
c. in the region outside the solenoids.
Assume that the thickness of current-carrying regions are negligible. Note that the magnetic field inside and outside an infinite solenoid with N turns of length L is Bvector = Bz * zhat, where Bz = 0 outside and Bz = μ0 * I * N / L inside its hollow interior.
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