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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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Why is the speed of DC shunt motor dependent on Back EMF?

A

Because flux is proportional to the armature current

B

Because armature drop is negligible

C

Because Back EMF is equal to armature current

D

Because flux is constant in DC shunt motor

Correct Answer

Concept & PrincipleElectricalElectric Drives
Option D

Because flux is constant in DC shunt motor

Quick Summary: In a DC shunt motor, the speed is directly dependent on the back EMF ($E_b$) and inversely proportional to the flux per pole ($\Phi$). Since the shunt field winding is connected in parallel with the armature across a constant supply voltage, the flux remains practically constant, making the back EMF the primary variable governing speed.

💡 Explanation

In a DC shunt motor, the speed is directly dependent on the back EMF (EbE_bEb​) and inversely proportional to the flux per pole (Φ\PhiΦ). Since the shunt field winding is connected in parallel with the armature across a constant supply voltage, the flux remains practically constant, making the back EMF the primary variable governing speed.

🔢 Key Formulas

N=KV−IaRaΦN = K \frac{V - I_a R_a}{\Phi}N=KΦV−Ia​Ra​​ — General speed equation for DC motors

Eb=PΦZN60AE_b = \frac{P \Phi Z N}{60 A}Eb​=60APΦZN​ — EMF equation of DC machine

⚙️ Working Principle

The fundamental speed equation is N=KEbΦN = K \frac{E_b}{\Phi}N=KΦEb​​. In a shunt motor, because the field is connected directly to the constant supply voltage, the field current Ish=VRshI_{sh} = \frac{V}{R_{sh}}Ish​=Rsh​V​ is constant, resulting in constant flux Φ\PhiΦ. Therefore, the motor speed NNN directly follows variations in EbE_bEb​, which is defined as Eb=V−IaRaE_b = V - I_a R_aEb​=V−Ia​Ra​. Any change in load affects IaI_aIa​, which in turn alters EbE_bEb​ to adjust the speed to the new equilibrium.

📌 Key Points
  • ▸

    Shunt motor acts as a constant speed motor due to constant flux excitation.

  • ▸

    Back EMF (EbE_bEb​) regulates the input current based on load demands.

  • ▸

    The armature voltage drop (IaRaI_a R_aIa​Ra​) is small, making Eb≈VE_b \approx VEb​≈V at no load.

  • ▸

    If the field circuit breaks, flux drops to near zero, causing speed to rise to dangerous levels (overspeed).

✅ Advantages
  • ▸

    Constant speed characteristic

  • ▸

    Easy to control speed via field rheostat

❌ Disadvantages / Limitations
  • ▸

    Low starting torque compared to series motors

  • ▸

    Not suitable for heavy traction applications

🛠️ Applications / Uses
  • ▸

    Centrifugal pumps

  • ▸

    Lathe machines

  • ▸

    Blowers and fans

📄 Additional Information
  • ▸

    Option A is incorrect because flux is independent of armature current in shunt motors.

  • ▸

    Option B is incorrect because while IaRaI_a R_aIa​Ra​ is small, it is critical for calculating EbE_bEb​.

  • ▸

    Option C is incorrect as EbE_bEb​ is a voltage, while IaI_aIa​ is a current, they cannot be equal.

📊 Diagram / Illustration
Speed Relation
N∝EbN \propto E_bN∝Eb​
Constant  ΦConstant \; \PhiConstantΦ
✅

D is correct — Because the shunt field is connected in parallel with the supply, the flux Φ\PhiΦ is held constant, forcing the speed NNN to be solely determined by the back EMF EbE_bEb​.

Core Concepts Used
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Back EMF Constant Flux Excitation DC Shunt Motor Characteristics
💡 EXAM TIP

Always remember: N∝EbΦN \propto \frac{E_b}{\Phi}N∝ΦEb​​. For shunt motors, Φ\PhiΦ is fixed; for series motors, Φ∝Ia\Phi \propto I_aΦ∝Ia​, which explains why shunt motors are 'constant speed' and series motors have 'high starting torque'.

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