Is the Back EMF of a Transformer a Dynamic Equilibrium?

In summary, the back emf of the primary coil always equal to the supply voltage but no greater than supply voltage. This is because there is a voltage drop across the resistance of the primary winding. If you apply Kirchhoff's voltage law to primary of the transformer, you get the back emf equal to supply voltage.
  • #1
haleycomet2
29
0
Why the back emf of the primary coil always equal to the supply voltage but no greater than supply voltage(because of the large number of coil turns) when no loaded?Or it is a kind of dynamic equilibrium?If yes,how it reach equilibrium?

Thank you.
 
Physics news on Phys.org
  • #2
haleycomet2 said:
Why the back emf of the primary coil always equal to the supply voltage but no greater than supply voltage(because of the large number of coil turns) when no loaded?Or it is a kind of dynamic equilibrium?If yes,how it reach equilibrium?

Thank you.

It is a simplifying assumption to assume that the back emf and supply voltage are the same.They are not exactly equal because there is a voltage drop across the resistance of the primary winding but usually this can be considered as negligible.
 
  • #3
If you apply Kirchhoff's voltage law to primary of the transformer, you get the back emf equal to supply voltage. (neglecting resistance in primary circuit)
 
  • #4
Under ideal condition(no resistance),since the back emf always equal to the supply voltage,then there would be no current flow through??
If different inductor(different L) is used in the circuit,does the dI/dt would be different even the supply voltage remains the same?
 
  • #5
haleycomet2 said:
Under ideal condition(no resistance),since the back emf always equal to the supply voltage,then there would be no current flow through??
If different inductor(different L) is used in the circuit,does the dI/dt would be different even the supply voltage remains the same?

There would initially be no current. But dI/dt is nonzero, so current will begin to flow according to the appropriate differential equation. The current will increase without bound if there's no limiting resistance; Better make sure there's some resistance in the circuit, or something's going to go FSSST-BANG!

If you change L, then you change the magnitude of dI/dt.
 
  • #6
ya,i just found it is clear when shown by differential equation.By the way, i am curious that is it possible to map out the trend of the unlimited increase of current?:smile:(let V is sin t and L is 1)
Thank you.
 
  • #7
haleycomet2 said:
ya,i just found it is clear when shown by differential equation.By the way, i am curious that is it possible to map out the trend of the unlimited increase of current?:smile:(let V is sin t and L is 1)
Thank you.

The worry about infinite increase in current applies to a constant voltage supply (or at least one with a constant, nonzero DC component).

If the supply is a sinewave, v(t) sin(t), then its integral over time is finite. So no blow-up for sinewaves!
 
  • #8
o...i see,thanks a lot..:approve:
 

1. What is back emf of a transformer?

Back emf (electromotive force) of a transformer is the voltage that is induced in the primary winding of a transformer due to the changing magnetic field created by the alternating current passing through the secondary winding.

2. Why is back emf important in a transformer?

Back emf is important in a transformer because it helps regulate the flow of current in the primary winding. When there is a high back emf, it can limit the amount of current that flows in the primary winding, preventing overheating and potential damage to the transformer.

3. How is back emf calculated in a transformer?

Back emf can be calculated by multiplying the number of turns in the secondary winding by the change in magnetic flux over time. This can be represented by the equation E = -N(dΦ/dt), where E is the back emf, N is the number of turns, and Φ is the change in magnetic flux over time.

4. What factors affect the back emf of a transformer?

The back emf of a transformer can be affected by factors such as the number of turns in the secondary winding, the frequency of the alternating current, and the strength of the magnetic field created by the secondary winding. Additionally, the amount of load on the secondary winding can also impact the back emf.

5. How can back emf be reduced in a transformer?

Back emf can be reduced in a transformer by using a lower frequency of alternating current, increasing the number of turns in the secondary winding, or decreasing the strength of the magnetic field created by the secondary winding. Additionally, using a load on the secondary winding can also help reduce back emf.

Similar threads

  • Introductory Physics Homework Help
Replies
3
Views
1K
Replies
10
Views
1K
  • Introductory Physics Homework Help
Replies
4
Views
979
  • Introductory Physics Homework Help
Replies
4
Views
2K
  • Introductory Physics Homework Help
Replies
8
Views
1K
  • Introductory Physics Homework Help
Replies
5
Views
1K
  • Introductory Physics Homework Help
Replies
2
Views
847
  • Introductory Physics Homework Help
Replies
5
Views
971
Replies
64
Views
5K
  • Introductory Physics Homework Help
Replies
3
Views
3K
Back
Top