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Chapter 1 of 12 • Page 1 of 248🔒 Protected PDF • Watermarked
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ElectricalElectric Drives
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The shaft torque (Tsh) in a d.c motor is less than total armature torque (Ta) because of ____________ in the motor.

A

Copper losses

B

Field Losses

C

Iron and Friction losses

D

None of the above

Correct Answer

Concept & PrincipleElectricalElectric Drives
Option C

Iron and Friction losses

Quick Summary: The shaft torque (T_{sh}) is the useful torque available at the motor shaft, whereas the armature torque (T_a) is the total torque developed by the armature. T_{sh} is less than T_a because rotational losses, comprising iron (hysteresis and eddy current) and mechanical friction/windage losses, consume a portion of the developed power.

💡 Explanation

The shaft torque (T_{sh}) is the useful torque available at the motor shaft, whereas the armature torque (TaT_{a}Ta​) is the total torque developed by the armature. T_{sh} is less than TaT_{a}Ta​ because rotational losses, comprising iron (hysteresis and eddy current) and mechanical friction/windage losses, consume a portion of the developed power.

🔢 Key Formulas

Ta=9.55EbIaNT_a = 9.55 \frac{E_b I_a}{N}Ta​=9.55NEb​Ia​​ — Total armature torque developed in Nm

Tsh=9.55PoutNT_{sh} = 9.55 \frac{P_{out}}{N}Tsh​=9.55NPout​​ — Useful shaft torque in Nm

Ta−Tsh=TlostT_a - T_{sh} = T_{lost}Ta​−Tsh​=Tlost​ — Torque lost due to mechanical and iron losses

⚙️ Working Principle

The electrical power converted into mechanical power is Pconv=EbIaP_{conv} = E_b I_aPconv​=Eb​Ia​. This power generates the armature torque Ta=PconvωmT_a = \frac{P_{conv}}{\omega_m}Ta​=ωm​Pconv​​. As this torque is transmitted through the shaft, energy is dissipated against frictional forces at the bearings and brushes, and aerodynamic windage losses occur. Additionally, iron losses in the core act as a retarding torque, reducing the net output torque to Tsh=Ta−TlostT_{sh} = T_a - T_{lost}Tsh​=Ta​−Tlost​, where TlostT_{lost}Tlost​ corresponds to the rotational losses.

📌 Key Points
  • ▸

    Armature torque (TaT_aTa​) is the total electromagnetic torque generated.

  • ▸

    Shaft torque (TshT_{sh}Tsh​) is the net torque available at the output shaft.

  • ▸

    The difference (Ta−TshT_a - T_{sh}Ta​−Tsh​) is known as lost torque or stray torque.

  • ▸

    Iron losses include hysteresis and eddy current losses in the armature core.

✅ Advantages
  • ▸

    Higher efficiency in larger machines

  • ▸

    Understanding these losses is crucial for accurate motor sizing

❌ Disadvantages / Limitations
  • ▸

    Rotational losses reduce the overall efficiency of the DC motor

  • ▸

    Increased thermal stress due to loss dissipation

🛠️ Applications / Uses
  • ▸

    Industrial motor design

  • ▸

    Drive performance evaluation

📄 Additional Information
  • ▸

    Copper losses (I2RI^2RI2R) affect the armature voltage drop and efficiency but are accounted for in the internal power conversion stage (EbIaE_bI_aEb​Ia​), making rotational losses the primary cause for the difference between internal developed torque and external shaft torque.

  • ▸

    Field losses depend on the field winding resistance and supply voltage, having minimal direct impact on the instantaneous torque conversion balance compared to rotational losses.

📊 Diagram / Illustration
Torque Relationship
Armature Torque (TaT_aTa​)
Shaft Torque (TshT_{sh}Tsh​)
- Rotational Losses
✅

C is correct — The shaft torque is lower than the armature torque because rotational losses (iron and friction) consume a part of the torque developed within the armature.

Core Concepts Used
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Electromagnetic Torque Rotational Losses Power Flow in DC Machines
💡 EXAM TIP

Always remember that TaT_aTa​ is internal to the armature and TshT_{sh}Tsh​ is the output; therefore, any loss occurring after the armature surface (mechanical) or within the core (iron) must result in a decrease in the delivered torque.

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