Solenoids PH 203 Professor Lee Carkner Lecture 18.
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Transcript of Solenoids PH 203 Professor Lee Carkner Lecture 18.
Magnetic Field: Solenoid What happens if you
stack several loops up?
You produce a solenoid
Field inside the solenoid is strong and uniform (far from the ends)
Solenoid Quantified We can write an expression for the
solenoid magnetic field:
B = 0ni
Note that: N is the total number of turns n = N/L
Toroid
The toroid has a radius r we can use as an Amperian loop
(B)(2r) = 0iN
B = (0iN)/(2r)
B is not constant and depends on where you are radially in the toroid
Magnetic Dipole
We can parameterize the loop with a dipole moment,
= NiA
If the loop is placed in an external magnetic field, it will experience a torque
= B sin where is the angle between and B
Dipole Torque
Use the right hand rule to find the direction of
Dipoles that are not aligned with the field will turn until they are
Dipole Energy
U = -B cos When aligned with the field
the energy is –B
When opposite the field the energy is +B
Field from a Dipole
A dipole is effected by external magnetic fields and also produces its own magnetic field
B = (0)/(2z3) Field falls off rapidly with z
A wire is carrying a current straight towards you. What is the direction of the magnetic field of the wire?
A) straight towards you
B) down
C) up
D) circling the wire in a clockwise direction
E) circling the wire in a counterclockwise direction
A horizontal wire is carrying a current straight north. What is the direction of the magnetic field directly above the wire and directly below the wire?
A) east, west
B) up, down
C) north, south
D) up, west
E) It depends on the magnitude of the current