Skip to main content

Capacitor Start Induction Motors

The construction of this type of motors is similar to the resistance split phase type. The difference is that in series with the auxiliary winding the capacitor is connected. The capacitive circuit draws a leading current, this feature used in this type to increase the split phase angle α between the two currents Im and Ist.
       Depending upon whether capacitor remains in the circuit permanently or is disconnected from the circuit using centrifugal switch, these motors are classified as, 
1. Capacitor start motor and       2. Capacitor start capacitor run motors
        The connection of capacitor start motor is shown in the Fig. 1(a). The current Im lags the voltage by angle Φm while due to capacitor the current Ist leads the voltage by angleΦst. Hence there exists a large phase difference between the two currents which is almost 90o , which is an ideal case. The phasor diagram is shown in the Fig.1(b).
Fig 1.  Capacitor start motor

       The starting torque is proportional to 'α 'and hence such motors produce very high starting torque .
       When speed approaches to 75 to 80% of the synchronous speed, the starting winding gets disconnected due to operation of the centrifugal switch. The capacitor remains in the circuit only at start hence it is called capacitor start motors.
Key point : In case of capacitor start capacitor run motor, there is no centrifugal switch and capacitor remain permanently in the circuit. This improves the power factor.
       The schematic representation of such motor is shown in the Fig. 2.
Fig. 2 Capacitor start capacitor run motor

       The phasor diagram remains same as shown in the Fig.1(b). The performance not only at start but in running condition also depends on the capacitor C hence its value is to be designed so as to compromise between best starting and best running condition. Hence the starting torque available in such type of motor is about 50 to 100% of full load torque.
       The direction of rotation, in both the types can be changed by interchanging the connection of main winding or auxiliary winding. The capacitor permanently in the circuit improves the power factor. These motors are more costly than split phase type motors.
       The capacitor value can be selected as per the requirement of starting torque, the starting torque can be as high as 350 to 400 % of full load torque. The torque-speed characteristics is as shown in the Fig.3.
Fig.3  Torque speed characteristic of capacitor split phase motor

Applications 
       These motors have high starting torque and hence are used for hard starting loads. These are used for compressors, conveyors, grinders, fans, blowers, refrigerators, air conditions etc. These are most commonly used motors. The capacitor start capacitor run motors are used in celling fans, blowers and air-circulations. These motors are available upto 6 kW.

Example : A 250 W, 230 V, 50 Hz capacitor start motor has the following impedances at standstill.
Main winding, Zm = 7 + j5 Ω
Auxiliary winding, Za = 11.5 + j5 Ω
       Find the value of capacitor to be connected in series with the auxiliary winding to give a phase displacement of  between the currents in two windings. Draw the circuit and phasor diagram for motor.

Solution : Let Xc be the capacitive reactance to be connected with auxiliary winding at start, as shown in the Fig. 1(a).
Fig. 1(a)

...              Za = 11.5 + j (5-Xc ) Ω
                     = 7 + j5 Ω = 8.6023
       Now  Ia and Im must have a phase difference of 90o.  Im will lag the voltage by 35.5376o hence Ia must lead the voltage by (90o- 35.5376o ) i.e. 53.4624o , as shown in the Fig 1(b).
Fig. 1(b)

       The phase angle of  Za is,
                   Φa =tan-1((5 - Xc )/11.5) = -53.4624o
Key point :As leads, the phase angle of i.e. must be negative hence taken as
                   tan(-53.4624o ) = (5 - Xc )/11.5 i.e.
                   -1.34956 = (5 - Xc )/11.5
..                  Xc = 20.52 Ω = 1/(2πfC)
..                  C = 1/(2π x 50 x 20.52) = 155.1217 μF

Comments

Popular posts from this blog

Practical Commutation

The e.m.f. induced in each coil of armature is alternating in nature. If load is connected, the current flowing will also be alternating. But the flow of current in a d.c. generator must be undirectional. This can be achieved by the use of commutator. When the armature conductors are under the influence of one pole they carry current in one direction whereas the current is reversed when the conductors are under the influence of other pole. This reversal of current takes place along the magnetic neutral axis. Fig. 1 Note : The reversal of current is likely to take place in short interval when a coil is short circuited by a brush so that transfer of current from one direction to other is carried out without any sparking. This process is called commutation.        Thus a process by which current in the short circuited coil is reversed while it crosses the MNA is called commutation. The time during which the coil remains short circuited is known as...

Demagnetising and Cross Magnetizing Conductors

The conductors which are responsible for producing demagnetizing and distortion effects are shown in the Fig.1. Fig. 1        The brushes are lying along the new position of MNA which is at angle θ  from GNA. The conductors in the region AOC = BOD = 2θ  at the top and bottom of the armature are carrying current in such a direction as to send the flux in armature from right to left. Thus these conductors are in direct opposition to main field and called demagnetizing armature conductors.         The remaining armature conductors which are lying in the region AOD and BOC carry current in such a direction as to send the flux pointing vertically downwards i.e. at right angles to the main field flux. Hence these conductors are called cross magnetizing armature conductors which will cause distortion in main field flux.        These conductors are shown in the Fig. 2 Fig. 2  ...

Winding Pitches

Now we will consider the definitions of different types of winding pitches, required in the design of the armature winding. 1.1 Back Pitch         The distance which is measured interns of armature conductors i.e. between top and bottom coil sides of a coil measured around the back of the armature i.e. away from the commutator is called back pitch and is denoted by . It is measured interms of coil sides. Note : Since it is difference between odd and even number, it is always odd number.        The size of the coil is decided by the back pitch. The back pitch is normally equal to coilsides per pole. It is shown for lap and wave type of winding in the Fig. 1. Fig. 1        The back pitch for the winding shown in the Fig. 1 is y b = 14 - 1 = 13 as coilsides 1and 14 are of coil number 1. 1.2 Front Pitch        It is defined as the distance measured between two c...