We use (x) when the magnetic field goes into the plane.
We use (.) when the magnetic field goes out of the plane.
F = qv x B
with magnitude:
F = qv B sin theta
F = force
q = charge
v = velocity
B = magnetic field
Whenever you use the right-hand rule, follow these steps:
Orient your hand so that your thumb points in the direction of the velocity v.
If the charge is negative, turn your thumb by 180 degrees.
Point your fingers in the direction of B.
The direction of FB will then be perpendicular to your palm.
F = ILB
with magnitude: F = BIL sin theta
F = force
B = magnetic field
I = current
L = length of conductor
B= μo I / 2πr
B = magnetic field
I = applied current
μo = permeability of free space
r = the distance from the wire where the magnetic field is calculated
The induced current will always flow in the direction that opposes the change in magnetic flux that produced it.
Emf = -N (ΔΦ/ Δt)
‘Emf’ = Induced voltage or electromotive force.
‘N’ = The number of loops.
‘Δϕ’ = Change within magnetic flux.
‘Δt’ = Change in time
Whenever a conductor is placed in a varying magnetic field, an electromotive force is induced. If the conductor circuit is closed, a current is induced, which is called induced current.
The induced emf in a coil is equal to the rate of change of flux linkage.
emf = − dΦ/ dt
emf = electromotive force
dΦ = change in magnetic flux
dt = change in time
It is created in three ways:
Changing the area of the loop of wire in a stationary magnetic field.
Changing the magnetic field strength through a stationary circuit.
Changing the angle between the magnetic field and the wire loop.
Motional emf is the electromotive force generated by the motion of a conductor through a magnetic field.
It is given by the equation
emf = Blv, where
B is the magnetic field strength
l is the length of the conductor
v is the velocity of the conductor
This phenomenon is used in various applications, such as electric generators and motors.