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Why locus of the current did not start from the origin (where X and Y-axis start) in the case of circle diagram of a three-phase induction motor?
due to stator and rotor copper loss
because its rotating device
even at no load. IM draw the No-Load Current (I0тАЛ) due to Mechanical Losses And Iron Losses
None of these
even at no load. IM draw the No-Load Current (I0тАЛ) due to Mechanical Losses And Iron Losses
In the circle diagram of a three-phase induction motor, the current locus does not start from the origin because even under no-load conditions, the motor draws a finite no-load current (I0тАЛ). This no-load current is required to establish the rotating magnetic flux (magnetizing component, ImтАЛ) and to supply core (iron) and mechanical friction and windage losses (working component, IwтАЛ).
In the circle diagram of a three-phase induction motor, the current locus does not start from the origin because even under no-load conditions, the motor draws a finite no-load current (I0тАЛ). This no-load current is required to establish the rotating magnetic flux (magnetizing component, ImтАЛ) and to supply core (iron) and mechanical friction and windage losses (working component, IwтАЛ).
I0тАЛ=Im2тАЛ+Iw2тАЛтАЛ тАФ No-load current magnitude
ImтАЛ=I0тАЛsin╧Х0тАЛ тАФ Magnetizing component responsible for main field flux
IwтАЛ=I0тАЛcos╧Х0тАЛ тАФ Core loss and mechanical loss component
Power┬аFactor┬аat┬аNo┬аLoad=cos╧Х0тАЛ=\frac{I_w}{I_0}$ \approx 0.1 \text{ to } 0.2$$ тАФ Typical low no-load power factor
When a 3-phase supply is connected to the stator, a rotating magnetic field is established. To sustain this field, the motor draws a magnetizing current (ImтАЛ) that lags the supply voltage by 90┬░. Simultaneously, the iron losses in the stator core and mechanical losses due to rotation require an active active current component (IwтАЛ) in phase with the voltage. The phasor sum of these two components gives the no-load current I0тАЛ=Im2тАЛ+Iw2тАЛтАЛ, shifting the starting point of the current locus vector away from the origin.
The no-load current I0тАЛ of a three-phase induction motor is relatively high, usually 30% to 50% of full-load current, due to the presence of an air gap.
The vertical offset from the X-axis represents the active power loss at no load (stator core loss + mechanical friction and windage loss).
The horizontal offset represents the reactive magnetizing component required to establish the air-gap flux.
Circle diagrams allow predetermination of motor performance (efficiency, power factor, slip, torque) without direct loading tests.
Provides a simple visual tool to analyze motor operation across all slip ranges.
Assumes constant parameters (stator/rotor resistance and reactance), which actually vary with saturation and temperature.
Less accurate for high-capacity machines due to non-linear magnetizing characteristics.
Used in electrical machine testing alongside No-Load and Blocked-Rotor tests.
Performance analysis and design verification of 3-phase induction motors.
Option A is incorrect because stator and rotor copper losses depend primarily on load current. Stator I2R loss at no load is small, and rotor copper loss at no load is negligible (sтЙИ0).
Option B is incorrect because being a rotating device explains why mechanical loss exists, but does not fully define the total no-load current which also includes iron/core losses and magnetizing reactive power.
The no-load power factor cos╧Х0тАЛ is very low (0.1 to 0.2) due to the predominant magnetizing component ImтАЛ required to overcome air gap reluctance.
C is correct тАФ The current locus starts at the tip of the no-load current phasor I0тАЛ, which accounts for iron losses, mechanical losses, and magnetizing flux even when no mechanical load is applied.
Remember that transformer no-load current is only 2%тИТ5% of rated current because of a continuous iron core, while induction motor no-load current is 30%тИТ50% of rated current due to the air gap.