How exactly does a transformer work?

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    Transformer Work
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Discussion Overview

The discussion revolves around the functioning of transformers, focusing on the principles of electromagnetic induction, the role of alternating current, and the application of various rules such as Fleming's Right Hand Rule and Lenz's Law. Participants explore theoretical explanations and clarify misconceptions related to the operation of transformers.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant explains that current in the primary coil generates a magnetic field, which induces a current in the secondary coil according to Lenz's Law.
  • Another participant questions the application of Fleming's Right Hand Rule, noting that the coil itself is not moving, but the magnetic field is changing.
  • A different participant suggests that the magnetic field should be considered as moving or changing relative to the coils, leading to a discussion about the direction of magnetic flux and its intersection with the coil.
  • Some participants argue that Fleming's rule is not applicable to transformers since there are no moving parts, emphasizing the importance of changing magnetic flux due to alternating current.
  • There is a discussion about the phase relationship between input current and voltage in transformers, with mentions of real and reactive power components.
  • One participant highlights that the alternating current is essential for the operation of transformers, as direct current would not induce the necessary magnetic flux changes.

Areas of Agreement / Disagreement

Participants express differing views on the relevance of Fleming's Right Hand Rule to transformer operation, with some arguing it is not applicable while others attempt to reconcile its use. There is no consensus on the best way to explain the induction process in transformers, indicating multiple competing views remain.

Contextual Notes

Participants discuss the implications of alternating versus direct current on transformer functionality, as well as the assumptions underlying the application of various electromagnetic principles. The discussion reflects a range of interpretations regarding the mechanics of electromagnetic induction in transformers.

lokifenrir96
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Hi, the explanation I have been given for how a transformer works is this:

The current flows through the primary coil, hence generating a magnetic field around the coil. Imagine that the coil is wrapped in the anticlockwise direction around the soft iron core (and hence current flows anticlockwise), then by the Right Hand Grip Rule, the north pole would point down. Since the soft iron core is square/rectangular, then by extending the magnetic field induced in the core around the core, one can see that the magnetic field now within the core runs anticlockwise as well.

By Lenz's Law, the current in the secondary coil will then flow so as to oppose this magnetic field which produced it in the first place. So the coil is wrapped in the clockwise direction (and so current flows clockwise around the core), and the magnetic field generated by the secondary coil now has north pole pointing down. So the magnetic field it induces in the core is clockwise, and is opposed to that generated by the primary coil.

That's great and all, but I don't really see how this can be explained using Fleming's Right Hand Rule? I see the magnetic field generated by the primary coil at a particular instant when the current is pointing in that direction to have an upwards direction since it is anticlockwise around the core. But the relative motion of the coil to the magnetic field is downwards.

So, by Fleming's Right Hand Rule, doesn't this mean the direction of magnetic field is PARALLEL to the direction of relative motion? So how does this induce an emf in the secondary coil in the first place? Or is there any other way to explain besides Lenz's Law?

Sorry if this was damn long... thanks!
 
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What do you mean by "the relative motion of the coil to the magnetic field is downwards"? What motion of the coil?
 
Like, when using FRHR, we need to know the direction of current through the coil, the direction of external magnetic field, and the direction of relative motion of the coil. Meaning how the coil is cutting across the magnetic field lines.

In this case, the coil itself isn't moving, but the magnetic field should be when it's expanding or collapsing? So I guess the RELATIVE motion is opposite to that of direction magnetic field is moving.

Like, if A is stationary and B is moving, then if you take B as stationary, RELATIVE to B, A is moving.
 
Ah ok I think I see what you are asking. The field should be moving or changing in a parallel direction to the coils as if they were moving and the fields were static. Is that correct?
Edit: If so, what's the problem? The field lines still intersect the coil at a 90 degree angle at every point in the wires.
 
Last edited:
Why invoke Fleming's rule? That is about induction of a voltage due to movement. There are no moving parts in a transformer. To discuss how a transformer works you need to look at the rate of change of magnetic Flux.
 
sophiecentaur said:
Why invoke Fleming's rule? That is about induction of a voltage due to movement. There are no moving parts in a transformer. To discuss how a transformer works you need to look at the rate of change of magnetic Flux.

There's an alternating current passing through the primary coil - so the flux is constantly changing - this induces a current in the secondary coil.

One of the most important aspects of how a transformer works, is the current needs to be alternating - alternating current = alternating magnet flux. It doesn't work if the current is DC.

With an electric generator/motor, you change the magnetic flux by moving the shaft of the motor - current flows through the coil. With the transformer, you change the magnetic flux.

With the transformer you don't have to worry about the right hand rule - the coils just need to be close enough together.
 
For a typical transformer, the input current in phase with the input voltage produces the output power, while the input current 90 degrees out of phase with the input voltage produces the reactive (inductive) excitation (V = L dI/dt).
 
Bob S said:
For a typical transformer, the input current in phase with the input voltage produces the output power, while the input current 90 degrees out of phase with the input voltage produces the reactive (inductive) excitation (V = L dI/dt).

This just HAS to be, because a resistive load on the secondary appears as a resistance across the primary. V and I have to be in phase for the primary.

I can't see why the RH rule ever came into this. RH rule involves Movement.
 
From Bob S
For a typical transformer, the input current in phase with the input voltage produces the output power, while the input current 90 degrees out of phase with the input voltage produces the reactive (inductive) excitation (V = L dI/dt).
sophiecentaur said:
This just HAS to be, because a resistive load on the secondary appears as a resistance across the primary. V and I have to be in phase for the primary.

I can't see why the RH rule ever came into this. RH rule involves Movement.
I am just pointing out that a transformer has two components of input current, both real power and reactive power components, and these two input currents are in phase quadrature.
 
  • #10
Oh yes, of course but the quadrature can be made vanishingly small. The real is as a result of actual power transfer.
 

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