Electrical Machines · Single-Phase Motors

Understanding the Single-Phase Induction Motor: Equivalent Circuit

Dr. Mithun Mondal BITS Pilani, Hyderabad Campus Electrical Machines

Demonstrative Video

SECTION 01

Equivalent Circuit

  • Single-phase motor conceptualized as single common stator winding, but two rotors revolving in opposite directions.

  • Equivalent circuit based on double-field revolving theory

Without Core Loss

  • The stator impedance: \(Z_1 = R_1 + j X_1\)

  • Each rotor impedance: \(r_2 + jx_2\)

  • \(r_2\) (rotor resistance), \(x_2\) (standstill reactance), and \(x_m\) (magnetising reactance) are half the actual values w.r.t stator (as referred to stator)

SPIM 11
Spim 11
  • Iron loss neglected so exciting branch has only \(x_m\)

  • Full values by capital letters and half-values by small letters

Under standstill condition,\(V_f = V_b\)
  • \[Z_f = \dfrac{jx_m\left(\dfrac{r_2}{s}+jx_2\right)}{\dfrac{r_2}{s}+j\left(x_m+x_2\right)}\]
    Impedance of forward running motor with
  • \[Z_b = \dfrac{jx_m\left(\dfrac{r_2}{2-s}+jx_2\right)}{\dfrac{r_2}{2-s}+j\left(x_m+x_2\right)}\]
    Impedance of backward running motor with
SPIM 11
Spim 11
  • Under standstill condition, \(V_f = V_b\)

  • Under running condition, \(V_f\) almost \(90-95\%\) of \(V\)

Total torque
  • \[P_g = \left(\dfrac{1-s}{s}\right) \cdot I_2^2R_2\]
    Power developed by the rotor :
  • \[T_g = \dfrac{1}{2\pi N} \left(\dfrac{1-s}{s}\right) \cdot I_2^2R_2\]
    is the rotor r.p.s, then torque is If
  • \[T_g = \dfrac{1}{2\pi N_s} \dfrac{I_2^2R_2}{s} = k \cdot \dfrac{I_2^2R_2}{s}\]
    , then Since
  • \[T_f = K \cdot \dfrac{I_2^2R_2}{s} \qquad T_b = -K \cdot \dfrac{I_2^2R_2}{(2-s)}\]
    Therefore, forward and backward torques are:
  • Total torque \(T=T_f+T_b\)

Advantages & Limitations
  • \[T_f = I_3^2\cdot r_2/s\]
    Forward torque in synchronous watts:
  • \[T_b = I_5^2 \cdot r_2/(2-s)\]
    Backward torque :
  • \[T = T_f - T_b\]
    Total torque:
  • SPIM 11
    Spim 11
  • core loss represented by \(r_c\) connected in parallel with \(x_m\)

  • Running condition: \(V_f >> V_b\)

  • Most of the iron-loss take place in forward motor \(I_w = P_i/V_f\)

SPIM 12
Spim 12
  • Advantages:

    • smaller in size and lighter in weight

    • cheaper in cost

    • highly efficient

    • requires less maintenance

    • have a longer life

    • can be designed in a variety of sizes

  • Limitations

    • For a given frame size and temperature, its output is only 50% of the three-phase induction motor

    • Not self-started

    • Have a lower power factor

    • Efficiency is lower

    • Do not have a starting torque

    • For the same power output, these motors are more expensive than three-phase induction motors.