Alternating Current Motor and its Application in Electrical Motor Vehicles

Alternating current motor
A n alternating current generator converts mechanical energy into electrical energy, an
alternating current generator consists of a rectangular coil of wire connected to slip rings. The
coil is rotated uniformly in a magnetic field. Carbon brushes which press against the slip rings
leads the induced current to an external circuit.
As the coil rotates an electromotive force is induced in both sides of the coil, since they cut the
magnetic field lines, it should be noted that no electromotive force will be induced that is parallel
to the magnetic fields lines, the electromagnetic force induced in edges of the coils depend on
their directions of motion relative to that of the magnetic field. At the instant the coil is vertical
and the edges that are perpendicular to the magnetic fields are moving to the direction that is
parallel to the magnetic and the induced electromagnetic force is zero. At the instant the coil is
horizontal and the direction of the motion of the edges is perpendicular to the magnetic field and
the induced electromotive force is maximum.
Suppose at an instant the plane of the coil is inclined at an angle θ to the vertical and the
perpendicular edges to the magnetic fields are moving with velocity v.
The components of velocity, v perpendicular and parallel to the direction of the magnetic field
are vsinθ respectively. Since e the induced electromotive force is proportion to the rate at which
the conductor cuts the magnetic flux, the induced electromotive force on the sides that are
perndicular to the magnetic field is proportion to the component of velocity of the edges
perpendicular to the magnetic field.
The induced e.m.f is thus proportion to vsin θ. Velocity v is constant and thereforce induced e.m.f
is proportion to sinθ. If maximum induced electromotive force is E0, then the induced
electromotive force E at any instant is given by E = E0* sinθ
Applying Fleming right hand rule, the induced current flows from right hand side towards the
left hand side, and the induced electromotive force will be observed to increase from zero to 900
then decreases to zero when the coil will be vertical.

Suppose E is the induced e.m.f at a given instant, E0 the maximum electromotive force and θ the
inclination of the coil to the vertical.
Then
E = E0* sinθ
By Ohms law
I = E
R
Where R is the resistance of the circuit
I is the current in the coil at any instant
I = E
R = E 0
R sinθ
If I0 is maximum value of I
Then I0 = E 0
R
And I = I0sinθ

Application of a direct current motor and alternating current motor on the automobiles
With machines that are brushless, it will contain a rotor which includes two or more permanent
magnets that generates a direct current magnetic field, the magnetic field will enter a core which
is made up of thin stacked lamination also known as stator core, it will then interact with current
that is flowing through the winding hence producing a torque interaction (Miller, 2004) that will
be between the rotor and stator. As the rotor is rotating the polarity and magnitude of the stator
current will be continuously be varying, in order to maintain the torque to be constant and the
conversion of electrical to mechanical energy to be highly efficient, the inverter will provides the
current control.
The induction rotor has a partial similarity ranging from three sets of distributed winding that are
inserted with the stator core, their different is only on the rotor, where the induction rotor lacks
magnet, having only a stack steel lamination together with is buried peripheral conductors,
current will flow in stator windings to produce a rotating magnetic field which is equivalent to
the different between the applied electrical frequency and the rotation frequency.
An induced voltage will exist a cross the shorted structure that will be proportional to the speed
difference that exist between the rotor and electrical frequency, in line with the existence of
voltage, current will be produced within the rotor conductors that are proportional to the voltage.
The interaction of the current with the magnetic field will produce force that is a component that
result to rotor torque.
The connection of a 3-phase induction motor to a 3-phase electrical power will result to
production of torque at the outset, the motor will only start under load, unlike the brushless direct
current motor that will produce no starting torque when it is connected to a fixed frequency
utility power, until there is the presence of inverter that maintains phase in step with angular
position of the rotor.