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ElectricalMachine
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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?

A

due to stator and rotor copper loss

B

because its rotating device

C

even at no load. IM draw the No-Load Current (I0I_0I0тАЛ) due to Mechanical Losses And Iron Losses

D

None of these

Correct Answer

тЪЩя╕П TE тАв Technical Concept & PrincipleElectricalMachine
Option C

even at no load. IM draw the No-Load Current (I0I_0I0тАЛ) due to Mechanical Losses And Iron Losses

Quick Summary:

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 (I0I_0I0тАЛ). This no-load current is required to establish the rotating magnetic flux (magnetizing component, ImI_mImтАЛ) and to supply core (iron) and mechanical friction and windage losses (working component, IwI_wIwтАЛ).

тЪЩя╕ПTETechnical SolutionConcept & Principle
ЁЯТб Explanation

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 (I0I_0I0тАЛ). This no-load current is required to establish the rotating magnetic flux (magnetizing component, ImI_mImтАЛ) and to supply core (iron) and mechanical friction and windage losses (working component, IwI_wIwтАЛ).

ЁЯФв Key Formulas

I0=Im2+Iw2I_0 = \sqrt{I_m┬▓ + I_w┬▓}I0тАЛ=Im2тАЛ+Iw2тАЛтАЛ тАФ No-load current magnitude

Im=I0sinтБб╧Х0I_m = I_0 \sin\phi_0ImтАЛ=I0тАЛsin╧Х0тАЛ тАФ Magnetizing component responsible for main field flux

Iw=I0cosтБб╧Х0I_w = I_0 \cos\phi_0IwтАЛ=I0тАЛcos╧Х0тАЛ тАФ Core loss and mechanical loss component

Power┬аFactor┬аat┬аNo┬аLoad=cosтБб╧Х0=\text{Power Factor at No Load} = \cos\phi_0 =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

тЪЩя╕П Working Principle

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 (ImI_mImтАЛ) that lags the supply voltage by 90┬░90┬░90┬░. Simultaneously, the iron losses in the stator core and mechanical losses due to rotation require an active active current component (IwI_wIwтАЛ) in phase with the voltage. The phasor sum of these two components gives the no-load current I0=Im2+Iw2I_0 = \sqrt{I_m┬▓ + I_w┬▓}I0тАЛ=Im2тАЛ+Iw2тАЛтАЛ, shifting the starting point of the current locus vector away from the origin.

ЁЯУМ Key Points
  • тЦ╕

    The no-load current I0I_0I0тАЛ of a three-phase induction motor is relatively high, usually 30%30\%30% to 50%50\%50% of full-load current, due to the presence of an air gap.

  • тЦ╕

    The vertical offset from the X-axis represents the active power loss at no load (stator core loss + mechanical friction and windage loss).

  • тЦ╕

    The horizontal offset represents the reactive magnetizing component required to establish the air-gap flux.

тЬЕ Advantages
  • тЦ╕

    Circle diagrams allow predetermination of motor performance (efficiency, power factor, slip, torque) without direct loading tests.

  • тЦ╕

    Provides a simple visual tool to analyze motor operation across all slip ranges.

тЭМ Disadvantages / Limitations
  • тЦ╕

    Assumes constant parameters (stator/rotor resistance and reactance), which actually vary with saturation and temperature.

  • тЦ╕

    Less accurate for high-capacity machines due to non-linear magnetizing characteristics.

ЁЯЫая╕П Applications / Uses
  • тЦ╕

    Used in electrical machine testing alongside No-Load and Blocked-Rotor tests.

  • тЦ╕

    Performance analysis and design verification of 3-phase induction motors.

ЁЯУД Additional Information
  • тЦ╕

    Option A is incorrect because stator and rotor copper losses depend primarily on load current. Stator I2RI^2RI2R loss at no load is small, and rotor copper loss at no load is negligible (sтЙИ0s \approx 0sтЙИ0).

  • тЦ╕

    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.

  • тЦ╕

    The no-load power factor cosтБб╧Х0\cos\phi_0cos╧Х0тАЛ is very low (0.10.10.1 to 0.20.20.2) due to the predominant magnetizing component ImI_mImтАЛ required to overcome air gap reluctance.

ЁЯУК Diagram / Illustration
V (Voltage Axis)I_active AxisO (Origin)IтВАIw (Losses)Im (Magnetizing)No-Load Point (A)Output Line Base
тЬЕ

C is correct тАФ The current locus starts at the tip of the no-load current phasor I0I_0I0тАЛ, which accounts for iron losses, mechanical losses, and magnetizing flux even when no mechanical load is applied.

Core Concepts Used
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Circle Diagram of Induction Motor No-Load Current Components ($I_m$ and $I_w$) Induction Motor Loss Analysis
ЁЯТб EXAM TIP

Remember that transformer no-load current is only 2%тИТ5%2\%-5\%2%тИТ5% of rated current because of a continuous iron core, while induction motor no-load current is 30%тИТ50%30\%-50\%30%тИТ50% of rated current due to the air gap.

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