Electrical motors are everywhere
around us. Almost all the electro-mechanical movements we see around us are
caused either by a AC or a DC motor.
Here we will be exploring DC motors. This is a device that converts DC
electrical energy to a mechanical energy.
This DC or direct current motor works on the
principal, when a current carrying conductor is placed in a magnetic field, it experiences a
torque and has a tendency to move.
This is
known as motoring action. If the direction of current in the wire is reversed,
the direction of rotation also reverses. When magnetic field and electric field
interact they produce a mechanical force, and based on that the working
principle of DC motor is established.
The direction of rotation of a this motor is given by Fleming’s left hand rule,
which states that if the index finger, middle finger and thumb of your left
hand are extended mutually perpendicular to each other and if the index finger
represents the direction of magnetic
field,
middle finger indicates the direction of current, then the thumb represents the
direction in which force is experienced by the shaft of the DC motor.
Structurally
and construction wise a direct current motor is
exactly similar to a DC
generator,
but electrically it is just the opposite. Here we unlike a generator we supply
electrical energy to the input port and derive mechanical energy from the
output port. We can represent it by the block diagram shown below.
Here in a DC motor, the supply voltage E and current I is given to
the electrical port or the input port and we derive the mechanical output i.e.
torque T and speed ω from the mechanical port or output port.
The input
and output port variables of the direct current motor are related by
the parameter K.
So from the picture above we can well understand that motor is just the
opposite phenomena of a DC
generator,
and we can derive both motoring and generating operation from the same machine
by simply reversing the ports.
To understand the DC motor in details lets consider
the diagram below,
The direct current motor is
represented by the circle in the center, on
which is mounted the brushes, where we connect the external terminals, from
where supply voltage is given. On the
mechanical terminal we have a shaft coming out of the Motor, and connected to
the armature, and the armature-shaft is coupled to the mechanical load. On the
supply terminals we represent the armature resistance Ra in
series. Now, let the input voltage E, is applied
across the brushes. Electric current which
flows through the rotor armature via brushes, in presence of the magnetic field, produces a
torque Tg . Due to this
torque Tg the dc motor armature
rotates. As the armature conductors are carrying currents and the armature
rotates inside the stator magnetic
field, it
also produces an emf Eb in
the manner very similar to that of a generator. The generated Emf Eb is directed
opposite to the supplied voltage and is known as
the back Emf, as it counters the forward
voltage.
The back emf like in case of a generator is
represented by
Where, P = no of poles
φ = flux per pole
Z= No. of conductors
A = No. of parallel paths
and N is the speed of the DC Motor.
So, from the above equation we can see Eb is
proportional to speed ‘N’. That is whenever a direct current motor rotates,
it results in the generation of back Emf.
Now lets represent the rotor speed by ω
in rad/sec. So Eb is
proportional to ω.
So, when the speed of the motor is reduced by the application of load, Eb decreases. Thus the voltage difference between supply voltage and back emf increases that means E − Eb increases. Due
to this increased voltage
difference,
armature current will
increase and therefore torque and hence speed increases. Thus a DC Motor is
capable of maintaining the same speed under variable load.
Now armature current Ia is represented by
Now at starting,speed ω
= 0 so at starting Eb = 0.
Now since the armature
winding electrical resistance Ra is small, this motor has a very high
starting current in the
absence of back Emf. As a result we need to use
a starter for starting a DC Motor.
Now as the
motor continues to rotate, the back Emf starts
being generated and gradually the current decreases
as the motor picks up speed.
Direct motors are named according to the connection o the
field winding with the armature. There are 3 types:
1. Shunt wound DC motor
2. Series wound DC motor
3. Compound wound DC motor