What Is Back EMF in DC Motors and How Does It Affect Performance?

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SUMMARY

Back EMF in DC motors is the voltage generated by the motor's rotation, opposing the applied voltage. In a series DC motor with an internal resistance of 2.00 Ω, operating at 120 V and drawing 4.00 A, the back EMF is calculated using the formula E = V - Ir, where I is the current and r is the resistance. The power delivered to the motor can be determined using P = I^2r, while the efficiency can be calculated based on the mechanical power developed versus the input power. When the motor stalls, the back EMF drops to zero, causing the entire applied voltage to contribute to the current flow.

PREREQUISITES
  • Understanding of Faraday's Law of Electromagnetic Induction
  • Knowledge of electrical circuit principles, specifically Ohm's Law
  • Familiarity with power calculations in electrical systems
  • Basic concepts of motor operation and efficiency
NEXT STEPS
  • Study the relationship between back EMF and motor speed in DC motors
  • Learn about efficiency calculations in electric motors
  • Explore the effects of load changes on DC motor performance
  • Investigate the implications of motor stalling and protective measures
USEFUL FOR

Electrical engineers, students studying motor dynamics, and anyone involved in the design or analysis of DC motor systems will benefit from this discussion.

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Homework Statement


A series dc motor:[/B] A dc motor with its rotor and field coils connected in series has an internal resistance of 2.00 Ω. When running at full load on a 120-V line, it draws a current of 4.00 A.

a) What is the emf in the rotor?
b) What is the power delivered to the motor?
c) What is the rate of dissipation of energy in the resistance of the motor?
d) What is the mechanical power developed?
e)What is the efficiency of the motor?
f)What happens if the machine that the motor is driving jams and the rotor suddenly stops turning?

Homework Equations


Vab = E + Ir,
P = I^2r

The Attempt at a Solution


This is a worked example in my textbook so the answers are all there but I'm finding it challenging to understand what is actually going on with some of the equations.

what exactly is the back emf and why am I adding it to Ir?

why does the current become V_ab/r only when the back emf goes to zero? what would be in the equation
I=v_ab/r if the back emf was still there?

would appreciate help with any of these questions and maybe an explanation of what is actually going on here. thanks
 
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The motor rotates. As a result, there are wires cutting through a magnetic field. This generates a voltage, according to Faraday's Law, and this is opposite to the applied voltage. The current that flow depends on the net voltage.
There are many analogues to this relationship. You can think of the back EMF as like inertia in kinetics, and the resistance like friction.
In chemistry, there's Le Chatelier's principle.
 
thank you. how come the emf and Ir are added together in this case and not subtracted if they are opposite? then when the motor stalls the total voltage of 120v is used in the equation? was it 8 before?
 
navm1 said:
thank you. how come the emf and Ir are added together in this case and not subtracted if they are opposite?
No, I said it opposes the applied voltage. Ir is then what's left after subtracting the back EMF from the applied EMF.
navm1 said:
then when the motor stalls the total voltage of 120v is used in the equation? was it 8 before?
Was what 8 before?
 

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