Need help understanding inductors

  • Thread starter Curious146
  • Start date
  • Tags
    Inductors
In summary: Education/AskExperts/ae73.cfmIn summary, an inductor resists changes in current due to its ability to store energy in the form of a magnetic field. When current is applied, the inductor initially acts as an open switch, causing the voltage to drop across it and opposing the applied voltage. As the current builds up, energy is stored in the inductor and it eventually reaches a steady state condition. This behavior can be explained through a differential equation and is a result of the fact that charge in motion is surrounded by a magnetic field, giving it a form of "inertia." The inductor serves to transfer electrical energy into the magnetic field, to be returned at a later
  • #1
Curious146
1
0
I'm having a hard time visualizing what is happening in an inductor and why it is happening. I understand the graphs and practical application but I can't seem to physically understand what is happening as you pass current through the inductor besides the fact that it builds a magnetic field. I think the relationship between the magnetic field and the circuit is confusing me.

If anyone could help me with a basic explanation of why an inductor resists change to current it would be greatly appreciated.
 
Engineering news on Phys.org
  • #2
Curious146 said:
I'm having a hard time visualizing what is happening in an inductor and why it is happening. I understand the graphs and practical application but I can't seem to physically understand what is happening as you pass current through the inductor besides the fact that it builds a magnetic field. I think the relationship between the magnetic field and the circuit is confusing me.

If anyone could help me with a basic explanation of why an inductor resists change to current it would be greatly appreciated.

Welcome to the PF, Curious.

At least for me, the basic inductor differential equation has helped me the most to feeling comfortable using them:

[tex]v(t) = L \frac{di(t)}{dt}[/tex]

So the voltage across an inductor is related to the change in the current through the inductor. This helps to explain the phase shift in voltage across inductors in circuit analysis problems, and also helps to understand the kickback voltage that is generated when you open a circuit that has an inductor carrying a current through it.
 
  • Like
Likes sophiecentaur
  • #3
This interactive image from the HyperPhysics website may give you ways to visualize the differential equation that berkeman provided and the physics behind it.

indcon.gif
 
  • Like
Likes berkeman
  • #4
di/dt is the change in current per unit time. It is key to understanding inductors.

When a current goes through an inductor it creates a magnetic field. You just need to accept that or watch some feynman physics lectures (well, youtube might have some videos, too) Creating that field required energy. When you initially apply voltage to an inductor, initially there is no field. The current slowly starts ramping up as the field is created. (di/dt is created by V based on the inductor size) The formation of the field resists (slows, or impedes) the growing current. An ideal inductor has no ohmic resistance so the current, and the field, can grow forever for any given V. If I stop the current from growing (which, strangely enough, leaves zero voltage across the inductor since di/dt is zero), the field is simply maintained. If I reduce the current, the field collapses some while trying to keep the current the same (and a voltage results).

So the basic action of an inductor is that it resists current changes through stored energy in its magnetic field. Increasing current is resisted by the growing field, decreasing current is resisted by the collapsing field.
If I stop the current altogether, I get a huge voltage as the field collapses and creates an infinite voltage to try to maintain the field.

v(t)=L di(t)dt basically means that applying a constant voltage causes a constant ramp in current (regulated by the increasing magnetic field).

To say it another way, the creation of a magnetic field induces current that impedes the growth of the field. The field changes cutting across the wires always resists the current that is creating or collapsing the field.

According to Lenz's law the direction of induced e.m.f is always such that it opposes the change in current that created it.
 
  • #5
meBigGuy said:
So the basic action of an inductor is that it resists current changes

Its important to get the terminology correct in the case of inductors.

Ideal inductors don't resist change in current; they oppose a change which is a crucial difference.

The total opposition to current in an AC circuit is impedance, or which resistance is just a part. Of course, in reality, all components have a resistive element, but this is a different process, and its important not to confuse the two, because very different results arise.
 
  • #6
Curious146 said:
I'm having a hard time visualizing what is happening in an inductor and why it is happening. I understand the graphs and practical application but I can't seem to physically understand what is happening as you pass current through the inductor besides the fact that it builds a magnetic field. I think the relationship between the magnetic field and the circuit is confusing me.

If anyone could help me with a basic explanation of why an inductor resists change to current it would be greatly appreciated.
Inductor stores energy in magnetic form. When you apply step voltage to an RL circuit, inductor acts as an open switch at that instant, causing all the voltage to drop across it. It opposes the applied voltage till the rate of change of current is 0 (almost), which depends on the time constant L/R. This behavior is best explained with a differential equation that you already know. As the current builds up, energy gets stored in the inductor and it finally becomes LI2/2 at the steady state. If you removed L from the circuit, the steady state would appear instantly after applying the voltage. But with inductor, it takes some time (in which the inductor stores energy) to reach the same steady state condition.
 
  • #7
Charge in motion is current
but unlike matter in motion, charge has no mass to establish inertia.

There's a quaint property of the universe that surrounds charge in motion with a magnetic field,
and that's where charge in motion stores its "inertia".

Mass in motion has kinetic energy ½ M v2
Charge in motion has energy (Kinetic or Potential? I'm unsure) ½ L I2
where L is inductance of the circuit, amount of magnetic flux per amp.
We can physically arrange the circuit to maximize inductance.

so what goes on in an inductor is: electrical energy is moved from the source into the magnetic field, to be returned at some later time.

magnetic field around a wire , courtesy http://hyperphysics.phy-astr.gsu.edu/hbase/magnetic/magcur.html

magcur.gif
arranging the circuit for more inductance
sol3.gif
any help ?

old jim
 
  • #8
Note to participants: please reserve inclusion of losses for another thread.

The goal in the present discussion is towards an understanding of pure inductance as a circuit element.
 
  • #9
Curious146 said:
If anyone could help me with a basic explanation of why an inductor resists change to current it would be greatly appreciated.

It was observed before it was figured out. Look up Lenz's law.

proxy.php?image=http%3A%2F%2Fhyperphysics.phy-astr.gsu.edu%2Fhbase%2Fmagnetic%2Fimgmag%2Fsol3.gif


Here is a simplistic explanation at the nuts & bolts level.

In this inductor, should current try to change because of something somebody did out there in the external circuit,
the magnetic field must grow or shrink.
As it does, the magnetic lines move outward or inward. As they cross the conductors they apply force to free charges inside the conductors. You do believe in QV cross B ?
Those forces, integrated along the length of the wire, make a voltage at the inductor's terminals that opposes the change in current.
(Search on Lenz's Law).

Now as you know, rate of change is slope on a graph ,
and rate of change of current of current is di/dt,
and the voltage across an inductor is L * di/dt

Sinusoids don't change shape when you differentiate them so it's not apparent by looking at them this derivative exists, all you see is phase shift.

Here's an actual 'scope photo of volts across an inductor with a triangle wave current

current above, ~20 ma p-p
voltage below , somewhat less than a volt p-p

f474b08e-86ad-46f5-aeb1-a360028b1a3c_zpsri5u078a.jpg

Triangle wave current has two distinct slopes
and (almost) square voltage wave has two distinct levels,
which to me is visual proof e = L di/dt.
(Rounded corners of squarewave are a secondary effect from imperfect iron core in this inductor. They weren't there with air core.)

The inductor does its best to keep current constant.

Curious146 said:
why an inductor resists change to current i

Same exact reason a flywheel resists change in rotation. Energy is conserved. Magnetic of the inductor field stores it .

There's probably an electrical analogy to gyroscopic properties of a flywheel too, but my vector calculus is too weak to explore that thought.

Any help? When your mind will work it like inertia, the formulas become intuitive.
Surely you've spun motors by hand and felt their inertia. The work you put in with your hand comes back out as force opposing your hand, not as heat. Energy is stored in the inertia for return later. Just like an inductor.

I oversimplify this way to help you over the same stumbling blocks i struggled past.
Work those differential equations and refine your mental model until the math flows naturally from it. That sure beats cramming for exams...

old jim
 
  • #10
jim hardy said:
There's probably an electrical analogy to gyroscopic properties of a flywheel too, but my vector calculus is too weak to explore that thought.
If it helps - I can offer another "analogy", which is even more than an anlogy:
We can replace the energy of the magnetic field by the energy of the E-field of a capacitor.

The background is as follows: There is an active electronic circuit involving two opamps which can mimic the behaviour of a passive one-sided grounded coil (inductor).
The core of this circuit is the so-called "generalized impedance converter (GIC)" which often is used as a replacement for an inductor in active filters and oscillator circuuits.
This GIC based active inductor consists of two equal opamps, 4 equal resistors and one capacitor and the "simulated" inductance is L=R²C (unit is Henry).
It has been prooved that this circuit can replace a grounded inductor in the time as well as in the frequency domain.
And the "inductive" behaviour of the circuit can be verified using the voltage storage capabilities of the capacitor.

PS: Keyword GIC can be found in wikipedia.
 
  • #11
LvW said:
There is an active electronic circuit involving two opamps which can mimic the behaviour of a passive one-sided grounded coil (inductor).
that's a handy circuit

i once used this one, from old National appnote AN31 ?

upload_2015-9-2_10-51-38.png


http://www.ti.com/ww/en/bobpease/assets/AN-31.pdf

but GIC is new to me...

if every day i learn something new, i should eventually know something.

old jim
 
  • #12
LvW said:
PS: Keyword GIC can be found in wikipedia.
Doesn't seem to be one. Do you have a link you like for GIC. Can it emulate ideal inductors? or is it someone limited like the Gyrator.
 
  • #13
I would love to change all instances of the word "resists" to "opposes" in my post #4 as suggested by William White in post #5. He is absolutely correct.

Yet another summary of that which precedes:

A growing field cuts through coil turns inducing a current that opposes the growing current that is causing the field. And vice versa: A shrinking field cuts through the coil turns and induces a current that opposes the reduction in current that is shrinking the field. The inductor naturally opposes any change in current. This causes it to impede AC currents (quantified as impedance).

Inductor Field energy increases or decreases with the square of the current. ½ L I2
The current change either requires that energy be supplied to the field (for increasing current) or be dissipated externally (for decreasing current).

When the current is shut off abruptly and completely, the ideal inductor will create an infinite voltage to maintain the current flow and dissipate its stored energy. Sparks will generally ensue.
 
  • Like
Likes jim hardy
  • #14
meBigGuy said:
Doesn't seem to be one. Do you have a link you like for GIC. Can it emulate ideal inductors? or is it someone limited like the Gyrator.
Sorry - you are right. I was of the opinion that wiki has a description. As it seems - that is not the case.
Here is a good link (GIC for an "ideal" inductor - as far as a real opamp does allow it):
http://forum.allaboutcircuits.com/attachments/gyrator-inductor-options-pdf.9108/

(Sorry - this works only if you are registered/logged into the site). Therefore, I have nclosed a pdf paper (active inductor on page 10).

Such a two-opamp circuit is often used in active filters (active realization of LRC structures).

A comment to Jim Hardy`s circuit: This is one version of a LOSSY inductor; however, I think it is an equivalent to a real inductor (coil) in the frequency domain only (sinusoidal signals in the time domain).
It does not mimic the true step response of a lossy inductor.
 

Attachments

  • ActiveL_FDNR_Leapfrog.pdf
    894.9 KB · Views: 847
Last edited:
  • #15
Hey Curious,

Basically, time varying magnetic flux through the inductor is generated by the time varying current (magnetic fields are generated by currents through wires and moving charges) flowing through the inductor (remember inductors only have an effect for time varying currents). We know from Faraday's law and Lenz's law that a voltage is induced across the inductor in such a way that it produces a current that opposes the change in the flux caused by the original changing current. Generally, Faraday's law and Lenz's law are axiomatic descriptions of nature but really there are more fundamental explanations for these phenomena based on special relativity. Basically, nature does not like changing magnetic flux/fields and generates EMFs (voltages) that resist these changing fluxes (and in turn resists the change in the current). Also, I think Jim's analogy to inertia for massive bodies is excellent and I never thought about it quite that way before.

Regards,
Matt
 
  • #16
Hi All,

Silly question here I'm sure. But.

Why does current not travel the shortest distance across an inductive coil (if the coils are physically touching and not insulated) instead of all the way through the coil.

Any insight.


Thanks.
 
  • #17
Bringitondown said:
Why does current not travel the shortest distance across an inductive coil (if the coils are physically touching and not insulated) instead of all the way through the coil.
In that case, you'd expect it would take the shortest/easiest path, and it will; the consequence being that it won't show the value of L you'd designed for. So because we need the current to follow the full path along the wire you must space the turns so each is separated from its neighbours by an air gap, or else coat the wire with another form of insulation.
 
  • #18
Thanks for the reply NascentOxygen,

So If the windings are touching in an Inductor, transformer, motor/generator etc they will always have a form of insulation?
What has thrown me is that in some pictures of the components stated it looks like there is no insulation, but from your reply I assume that there would be some sort of clear insulating varnish or something similar.

Thoughts?

Thanks
 
  • #19
eg.

inductors.png
audio_inductor_ferrite_core_falcon_acoustics_super_super_power_ssp125_16.jpg
 
  • #20
Bringitondown said:
not insulated

As NO says, they are generally insulated. "Magnet Wire" has very thin insulation, since the voltage between adjacent turns is usually low. You can get magnet wire with standard thin insulation, or with "double build" or "triple build" insulation thicknesses, if you need more insulation or if you need the extra physical strength (with very fine magnet wire).
 
  • #21
Smashing thanks for clearing that up. I don't like to leave things to assumption.
 
  • #22
Bringitondown said:
What has thrown me is that in some pictures of the components stated it looks like there is no insulation, but from your reply I assume that there would be some sort of clear insulating varnish or something similar.
The transparent varnish is termed "enamel". Motors, relays and other electromagnets are wound using such enamelled copper wire.
 
  • #23
The volts between adjacent turns are very low so thin enamel coatings are sufficient and allow close packing. I believe that the layers are sometimes separated by an insulating tape as the volts will be n times what's between adjacent turns. (nV volts for n turns per layer). It's a very practical business.
 
  • #25
The poor OP seems to have withdrawn. Perhaps the responses were too weighty. I do wish questioners would respond to the first few answers so that people have a chance to pitch their replies at an appropriate level.
 
  • #26
sophiecentaur said:
I do wish questioners would respond to the first few answers so that people have a chance to pitch their replies at an appropriate level.
Probably why the thread got stickyed. :approve:
 

1. What is an inductor and how does it work?

An inductor is an electrical component that stores energy in the form of a magnetic field. It consists of a coil of wire, which creates the magnetic field when current flows through it. The ability of an inductor to store energy is known as inductance, and it is measured in henries (H). When the current flowing through an inductor changes, the magnetic field also changes, which in turn induces a voltage in the circuit.

2. What is the purpose of an inductor in a circuit?

An inductor has several purposes in a circuit, including filtering out unwanted signals, smoothing out variations in current or voltage, and regulating the flow of current. It can also be used to store energy and release it when needed, such as in the case of a surge protector.

3. How does the value of inductance affect the behavior of an inductor?

The value of inductance determines how much energy an inductor can store and how quickly it can release that energy. A higher inductance means a stronger magnetic field and a longer time for the current to reach its maximum value. This can lead to a delay in the current reaching its steady state and can also affect the frequency response of the inductor.

4. What factors affect the inductance of an inductor?

The inductance of an inductor depends on several factors, including the number of turns in the coil, the size and shape of the coil, the type of core material used, and the presence of nearby conductors or magnetic fields. The material and size of the wire used in the coil also play a role in determining the inductance.

5. How can I calculate the inductance of an inductor?

The inductance of an inductor can be calculated using the formula L = μN^2A/l, where μ is the permeability of the core material, N is the number of turns in the coil, A is the cross-sectional area of the coil, and l is the length of the coil. There are also online calculators and software programs available to help with inductance calculations.

Similar threads

Replies
4
Views
928
  • Electrical Engineering
2
Replies
38
Views
4K
Replies
25
Views
1K
Replies
4
Views
2K
  • Electrical Engineering
Replies
5
Views
3K
  • Classical Physics
Replies
14
Views
2K
  • Electrical Engineering
Replies
6
Views
3K
  • Electrical Engineering
Replies
10
Views
4K
  • Introductory Physics Homework Help
Replies
16
Views
182
  • Introductory Physics Homework Help
Replies
5
Views
204
Back
Top