Understanding Induced Current and EMF in Electromagnetic Induction

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In summary: It's a good thing to get the terminology right in things like this.An EMF doesn't "flow"; it is a Potential Difference and exists 'across' to parts of a circuit. A current will flow as a result of an applied potential difference. In Summary, an EMF opposes the change in flux, so if there is no current flowing an EMF will be induced.
  • #141
jsmith613 said:
Ok so I think you are saying that the mean emf will be zero but the mean current WILL NOT BE otherwise the magnetic field would not be produced, right?
??
As far as I'm concerned, as long as you ignore inductance (which you can), the current flowing in the coil of the tube will be directly proportional to the EMF. Where have I given the impression that they don't precisely track each other?

If current is flowing one way (because the emf is causing it to) in one part of the tube and in another direction in another part of the tube (for the same reason) then the mean current is zero but that doesn't imply that the Force on the magnet will be zero, does it? The currents at either end of the magnet must flow in opposite directions or the effect on one of the poles would be to PUSH the magnet down.

Are you reading elsewhere about Induction, RH and LH rules etc.? It may be a good idea because I think you may be mis-reading what I am writing at times. If you read someone elses way of putting things then perhaps it will make more sense to you.

All this stuff is so basic that it is available to read about all over the net. Have you ever tried the 'Hyperphysics ' pages? They are very good. I usually find something there for pretty well every topic.
 
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  • #142
sophiecentaur said:
If current is flowing one way (because the emf is causing it to) in one part of the tube and in another direction in another part of the tube (for the same reason) then the mean current is zero but that doesn't imply that the Force on the magnet will be zero, does it? The currents at either end of the magnet must flow in opposite directions or the effect on one of the poles would be to PUSH the magnet down.
ok thanks. I just wanted to check. I figured if the mean emf was zero and the mean current was zero I presumed no opposing magnetic forces would act. apparently this was wrong

sophiecentaur said:
Are you reading elsewhere about Induction, RH and LH rules etc.? It may be a good idea because I think you may be mis-reading what I am writing at times. If you read someone elses way of putting things then perhaps it will make more sense to you.
Before I started this discussion I looked endlessly over the internet (including Hyperphysics, Wiki) for relevant infromation but as I am only studying A2 Level physics (and don't really want to study more complicated physics than this) I could not find anything.
The A2 websites were not detailed enough and other websites were too detailed.
its a hard balance
 
  • #143
A level is strange these days. They spread the net wide and give you a taste of all sorts of new Physics topics*. This means you are spread much more 'thin' than when I did A level. I think it is bad for you because the course books never go far enough if you happen to get an interest in one particular topic. Have you access to a 'proper' textbook that was published a few years ago? You will probably find much better treatment of topics you find difficult. But you're talking £30+ rather than £10+ for a coursebook.The way to get good grades it just to LEARN every fact and formula in the specification (download it if you haven't yet) and then follow, step by step, the Exam questions, doing exactly what they ask. Needless to say, you have to be absolutely rock solid on the simple algebraic manipulation rules (re-arranging equations and the like) and the basic Trig formulae. That's where a lot of students are shaky.

*On the course that I taught (retired recently) they started AS Physics by talking about Fundamental Particles - loads of brand new ideas: "Particle Zoo" long before they dealt with how an electron behaves in an electric field. None of the students got anything out of it except the feeling that they 'knew about' some sexy particles. Totally fragmented.
 
  • #144
sophiecentaur said:
A level is strange these days. They spread the net wide and give you a taste of all sorts of new Physics topics*. This means you are spread much more 'thin' than when I did A level. I think it is bad for you because the course books never go far enough if you happen to get an interest in one particular topic. Have you access to a 'proper' textbook that was published a few years ago? You will probably find much better treatment of topics you find difficult. But you're talking £30+ rather than £10+ for a coursebook.The way to get good grades it just to LEARN every fact and formula in the specification (download it if you haven't yet) and then follow, step by step, the Exam questions, doing exactly what they ask. Needless to say, you have to be absolutely rock solid on the simple algebraic manipulation rules (re-arranging equations and the like) and the basic Trig formulae. That's where a lot of students are shaky.

well I am very good at maths (and do A2 maths).
I despise the way A-levels are structured...although the system is very easy to play with it means I come out not really knowing a lot of physics...i think this is why i dislike physics as a subject...the separate bits are fascinating but the way it is taught at A2 level means I learn some facts and just have to accept them.

anyway I would very much like to thank you and BruceW and everyone else who has helped me with this topic..hopefully if a question comes up I will be able to nail it :)
 
  • #145
jsmith613 said:
well I am very good at maths (and do A2 maths).
I despise the way A-levels are structured...although the system is very easy to play with it means I come out not really knowing a lot of physics...i think this is why i dislike physics as a subject...the separate bits are fascinating but the way it is taught at A2 level means I learn some facts and just have to accept them.

anyway I would very much like to thank you and BruceW and everyone else who has helped me with this topic..hopefully if a question comes up I will be able to nail it :)

That's a good start!

That's because the course is aimed at 'bums on seats' and supposed to be attractive. I don't know how you got on at GCSE in Science but I know that very few of the students who chose Physics at A/AS had a clue about what they were letting themselves in for. It 'sounds good' as a subject (and of course it is) but it demands a level of rigour, even at A level, which many students have never come across before. As a consequence of student responses to past exam questions, the structure of the course has been adjusted to be suitable for students who don't particularly 'want to think'. Giving lots of taster units and not concentrating on some serious basics means that, as you say, you are given stuff which you have to accept as a fact and can answer questions adequately by just remembering the what, rather than the how. Way back, the topics we were taught were very conventional (heat, light, sound + elec) but, even in the first year, we got the message about how important the 'book-work' was. We had to be able to derive all the basic equations (of which there were a lot) and to REMEMBER them (not a single A level formula was given on the paper - just the constants). I have always told my students that if they need to look up a formula then they can't actually be sure that they will use it properly - after all, they are all pretty straightforward.
Having had my rant, however, I reckon that, if your Maths is good and you are interested enough to be worrying this particular topic to death (haha), then you should do all right. If and when you get to Uni to do Physics then you will find it is more suited to your attitude, I think.
 
  • #146
jsmith613 said:
well I am very good at maths (and do A2 maths).
I despise the way A-levels are structured...although the system is very easy to play with it means I come out not really knowing a lot of physics...i think this is why i dislike physics as a subject...the separate bits are fascinating but the way it is taught at A2 level means I learn some facts and just have to accept them.

anyway I would very much like to thank you and BruceW and everyone else who has helped me with this topic..hopefully if a question comes up I will be able to nail it :)
Thanks, jsmith! I'm from uk too, and I recently finished my undergraduate physics degree. I'd say that A-level physics is a pretty good introduction to undergraduate-level physics (in case you're interested in doing that). The main difference is in how much maths goes on. There is definitely more maths involved in undergraduate physics than in A-level physics. And I think this is one of the main reasons that you must just accept some facts at A-level, because they simply haven't taught you the relevant maths yet. Also, they are trying to give you a broad view of physics, so it would take too long to go into detail.
 
  • #147
sophiecentaur said:
??
If current is flowing one way (because the emf is causing it to) in one part of the tube and in another direction in another part of the tube (for the same reason) then the mean current is zero but that doesn't imply that the Force on the magnet will be zero, does it? The currents at either end of the magnet must flow in opposite directions or the effect on one of the poles would be to PUSH the magnet down.

I would very much like to check I have understood this topic:
here is the summary of the way I see everything working in relation to the COIL (I am ignoring the tube as it seems more complicated than needed for A-level)

is this summary correct

the net emf (across the entire coil) is zero when the magnet is in the coil so the current in the coil is also zero...but the current at either end of the magnet (above and below it) is creating an instantaneous magnetic field opposing the motion of the magnet as it falls (due to the currents that are present - i.e: before they cancel). This is for when the oscilliscope is attached - it completes the circuit

if we remove the oscilloscope then no current can flow as there is no complete circuit..hence there will be no opposing magnetic field and the magnet will accelerate due to gravity with no opposing forces AT ALL TIMES..

I really hope this is correct

NOTE: I will not be able to sign in until Sunday as I have a busy weekend so I will not respond to any comments until then. I would still be delighted for people to comment:)
 
  • #148
Sort of... but an oscilloscope has 10Mohm resistance so you can say that no current flows!. If you were to short the ends together, you might get enough current to produce a measurable braking effect.
 
  • #149
sophiecentaur said:
Sort of... but an oscilloscope has 10Mohm resistance so you can say that no current flows!. If you were to short the ends together, you might get enough current to produce a measurable braking effect.

so it would be more correct to say that no breaking effect occurs inside the coil
but as it enters / leaves we will get current and hence breaking effect?
(inside the tube we DO get breaking effect due to eddy currents though, right)
 
  • #150
BruceW said:
Thanks, jsmith! I'm from uk too, and I recently finished my undergraduate physics degree. I'd say that A-level physics is a pretty good introduction to undergraduate-level physics (in case you're interested in doing that). The main difference is in how much maths goes on. There is definitely more maths involved in undergraduate physics than in A-level physics. And I think this is one of the main reasons that you must just accept some facts at A-level, because they simply haven't taught you the relevant maths yet. Also, they are trying to give you a broad view of physics, so it would take too long to go into detail.

The problem is that you start your A level course with GCSE Maths and not O level Maths, as I did and many people have just done Science GCSE Double Award. That effect trickles up all the way up to Degree level and this is why people are needing Masters Degrees to get the same cred as a good Hons degree in the dim and distant past. I guess, as all you young people are going to live till 100, an extra year doesn't actually hurt anyone. It's just the Politicians (****rds) who claim that kids are getting brighter as a result of their loony policies. Don't get me started on Synthetic Phonics. Grrrrr!
 
  • #151
jsmith613 said:
so it would be more correct to say that no breaking effect occurs inside the coil
but as it enters / leaves we will get current and hence breaking effect?
(inside the tube we DO get breaking effect due to eddy currents though, right)

Only if there is a connection between the two ends of the coil. A scope won't make it happen. What path could the current take?
 
  • #152
sophiecentaur said:
Only if there is a connection between the two ends of the coil. A scope won't make it happen. What path could the current take?

Displacement current due to end to end capacitance of the coil. Once again, I hate to keep saying this, because it should be very well known. In the ac domain, we MUST DISCARD this archaic notion that in order for current to exist that a fully closed path is required. A single conductor open at both ends can and does carry a current.

I apologize for being repetitive, but this should be so well known that it needn't be necessary to remind everyone. Of course, this displacement current, depending on conditions like speed, frequency, etc. may be too small to be concerned about. In the case of the car, that is likely the case.

Also, you earlier mentioned that the scope connected in mid air can measure voltage using short dipoles. Please refer to any reference text and it will affirm that the routing of the leads will affect the reading displayed. When measuring voltage (or emf) due to time varying magnetic fields, the geometry of the leads determines the enclosed area and path of integration. This affects emf value.

Also, the integral E*dl is used to evaluate emf, but it is derived as follows. The work done transporting charge along a given path is the integral F*dl. Voltage is defined as work per charge. So emf is the integral of (F*dl)/q. But F/q is simply E, so we write integral E*dl. But there is a restriction.

If q = 0, then F/q is undefined. What is the work transporting no charge around a given path? Answer is zero. What is the charge? Answer is zero. What is the voltage/emf? Answer is work divided by charge which is 0/0! In math 0/0 is known as indeterminate. It is undefined. Although integral E*dl is defined, work/charge is 0/0. Integral E*dl is derived from integral (F*dl)/q, which is the most fundamental since work/charge is the very definition of voltage.

Anyway, I had to clarify that in space with time changing fields, I think emf has meaning only in the presence of charges,and path is defined by the conductor. To remove both and discuss a voltage value in empty space results in amiguous and indeterminate voltage values. Anyway, that's how voltage is defined. Like I said, under static conditions we can indeed define a voltage value in free space w/o charges and/or conductors if the fields are conservative. In this case they voltage is independent of path of integration.

The conditions and nature of the fields need to be considered. When quoting an equation, such as integral E*dl, we must know how it was derived, and the conditions where it applies. Math and science is typically applied this way. Comments welcome.

Claude

Claude
 
  • #153
jsmith613 said:
the net emf (across the entire coil) is zero when the magnet is in the coil so the current in the coil is also zero...but the current at either end of the magnet (above and below it) is creating an instantaneous magnetic field opposing the motion of the magnet as it falls (due to the currents that are present - i.e: before they cancel). This is for when the oscilliscope is attached - it completes the circuit
When the magnet is in the middle of the coil, you are right that there is zero emf across the entire coil. But there is no current above or below the magnet (even if you 'short the ends together'). Remember that the current must be in the same direction over the entire coil, otherwise you'd get charge separation. (I am assuming here that the coil is too thin to allow significant eddy currents, which is the reason for using a coil in this experiment in the first place).

When the magnet is above the middle of the coil, the current will flow anticlockwise. This movement of charge will decrease the rate of change of flux below the magnet, but will increase the rate of change of flux above the magnet. But because the magnet is nearer the top half of the coil, the effect of the current flowing above the magnet is less than the effect of the current flowing below the magnet, so overall the rate of change of flux is decreased.

From this explanation, you can see that the braking effect will be zero when the magnet is in the middle of the coil, since there is as much coil above as there is below, so if there was a current, it would have no effect on the magnet's motion. So when the magnet goes through the middle of the coil, there is zero current. This is handy, since we know that once the magnet is below the middle of the coil, the current must be in the opposite direction to before. So it means that the current changes continuously from one direction to the other as the magnet passes through the coil.

When a magnet goes through a tube, the situation is different because eddy currents can exist, so the current can be different in different places in the tube. So the braking effect can exist even when the magnet is in the middle of the tube.

I hope this explanation has been of some help. To be honest, the most important thing is to get yourself ready for the kind of questions they will ask you (by reading past papers and practice questions). I guess you've done that and you're now looking to understand it more. And that is good, if they ask you an unexpected question, you will have an edge over other students.
 
  • #154
cabraham said:
Also, the integral E*dl is used to evaluate emf, but it is derived as follows. The work done transporting charge along a given path is the integral F*dl. Voltage is defined as work per charge. So emf is the integral of (F*dl)/q. But F/q is simply E, so we write integral E*dl. But there is a restriction.

If q = 0, then F/q is undefined. What is the work transporting no charge around a given path? Answer is zero. What is the charge? Answer is zero. What is the voltage/emf? Answer is work divided by charge which is 0/0! In math 0/0 is known as indeterminate. It is undefined. Although integral E*dl is defined, work/charge is 0/0. Integral E*dl is derived from integral (F*dl)/q, which is the most fundamental since work/charge is the very definition of voltage.
The integral E*dL is more fundamental than work per charge. It can be derived from Maxwell's equations, which do not require charges (the equations still work in free space).
[tex]\nabla \wedge \vec{E} = - \frac{\partial \vec{B}}{\partial t} [/tex]
[tex]\int ( \nabla \wedge \vec{E} ) \cdot d \vec{A} = - \frac{\partial \int \vec{B} \cdot d \vec{A}}{\partial t} [/tex]
[tex] \oint \vec{E} \cdot d \vec{L} = - \frac{\partial \Phi}{\partial t} [/tex]
So if you define emf as E*dL, the definition does not require charges. But if you define emf as (F*dL)/q then the definition does require some kind of charge to exist. It just depends on which definition you prefer.

EDIT: woops, I forgot it should be partial differential with respect to time, keeping spatial coordinates constant. I've changed it to partial derivative symbols now.
 
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  • #155
BruceW said:
The integral E*dL is more fundamental than work per charge. It can be derived from Maxwell's equations, which do not require charges (the equations still work in free space).
[tex]\nabla \wedge \vec{E} = - \frac{d \vec{B}}{dt} [/tex]
[tex]\int ( \nabla \wedge \vec{E} ) \cdot d \vec{A} = - \frac{d \int \vec{B} \cdot d \vec{A}}{dt} [/tex]
[tex] \oint \vec{E} \cdot d \vec{L} = - \frac{d \Phi}{dt} [/tex]
So if you define emf as E*dL, the definition does not require charges. But if you define emf as (F*dL)/q then the definition does require some kind of charge to exist. It just depends on which definition you prefer.

F/q is more basic than E. Force, F, can be observed between two charged bodies. But for this force to be felt, proagation time was observed. The field concept was created. By definition E field is a mathematical construct defined as F/q. Voltage was defined as work per unit charge even before fields were born. What is the voltage in an ac field if there is no charges nor conductor?

Per the definition of what voltage is, force per charge, it 0/0, which is indeterminate. But as soon as you introduce a conductor which posesses mobile charge carriers, all makes sense. You can then compute the work done per unit charge along a path which is defined by the size & shape of the conductor.

Since E was born out of the condition "F/q", we must apply the rules of math and stipulate the q can never equal 0. Otherwise we have no sense at all. That is my point. What is the work per charge along this path? No work is done moving no charge. Hence 0/0 is the only answer one can obtain. What is "0/0"? I don't know. I doubt anyone can know. I'm not trying to belabor this point, please understand that I just don't like things like "0/0". It doesn't sit right with me.

If you feel ok with defining a voltage in mid air which computes to "0/0", well who am I to argue? I just hope we can all agree that expressions like 1.3/24.6, -3.73/1.27, 0/1.52, etc., make sense, whereas "0/0" just doesn't do it for me. Am I being unreasonable here? Comments welcome.

Claude
 
  • #156
cabraham said:
F/q is more basic than E. Force, F, can be observed between two charged bodies. But for this force to be felt, proagation time was observed. The field concept was created. By definition E field is a mathematical construct defined as F/q. Voltage was defined as work per unit charge even before fields were born. What is the voltage in an ac field if there is no charges nor conductor?
The concept of a field is still useful in free space, without charges or currents. For example, if we were interested to know about how a radiation-dominated universe would evolve. I think our own universe was radiation-dominant for a while, if I remember right.
 
  • #157
BruceW said:
The concept of a field is still useful in free space, without charges or currents. For example, if we were interested to know about how a radiation-dominated universe would evolve. I think our own universe was radiation-dominant for a while, if I remember right.

Of course, a field is useful in free space. Fields were conceived to deal with the issue of propagation delay. Before the Coulomb force between 2 charges can take place, a disturbance, wave, field, whatever, had to propagate through space in the interim.

In free space there are definitely fields involved. But when we try to define a "work done per unit charge", i.e. "voltage", we run smack into that darn "0/0" indeterminate monster. But if we simply define a conductive path and introduce a very small quantity of charge, all is well.

When I think about it, what value does the voltage concept have if there are no conductors or charges? The whole concept of voltage is only useful when we observe charges moving under the influence of a field. Without charges and conductors, the fields are still there, but they have nothing to move. So the "work done divided by the charge" is literally 0/0!

But we seem to have resolved that E & B are always present even w/o conductors and/or charges. I don't think anybody would dispute that. I certainly don't, BR.

Claude
 
  • #158
@cabraham
You presumably don't subscribe, either, to the concept of a field then - which is a force on a mass / charge / current. The same "0/0" applies if the mass / charge / current isn't there? Is the field really not there when there's nothing to experience it? That's all a bit Zen for me, I'm afraid.

Did you do any calculation about who much this displacement current would be? I wonder if it is really relevant in the world of an A Level student really significant in comparison with the current that would flow if the two ends of a coil were joined together. I think you are allowing your preference for the way in which you choose to look at things to take over from a pragmatic approach that is used in most occasions where induction takes place.
[edit] Having just read your last post, I take it you don't subscribe, either, to the concept of Gravitational Potential?
 
  • #159
Just the opposite, I ascribe to fields in vacuum, and to a limited extent potentials in vacuum. Please reread. It's a question of how to compute/define. I can say that my opponents choose to view things in their preferred perspective. I'm just saying that voltage & current are equally important, neither one more or less than the other. In ac, neither is independednt nor causal or effectual. In dc, either one can exist alone. That is my point.

Claude
 
  • #160
So, after all this, we are down to a matter of preference. We have also risked really confusing a poor A level student over whose head all this has sailed (I hope).
I think a separate thread would have been appropriate for this discussion of angels on pinheads.
 
  • #161
Also, FWIW, I do ascribe to gravitational potential. Remember that gravity is a conservative field. As such, it can be equated to the negative of the gradient of a scalar potential function. The potential at any point in space due to gravity is well-defined, computable as a unique single value, independent of path.

Likewise with an E field due entirely to charged particles the same scenario exists. Take a parallel plate capacitor with charge on the plates. The potential anywhere between the plates is well defined and path INdependent. THe field is IRrotational just like gravity. Also, E = -grad V, like gravity.

Now when dealing with rotational E fields, like that with induction, E is NOT the gradient of a potention scalar function. Across any 2 points in space, there is no single valued potentiol. Potential, or emf, have meaning only along a specific path of charge motion, i.e. charges moving through a conductor under the influence of fields per the Lorentz force equation. Here, E = -dA/dt, where A is magnetic vector potential.

Rotational fields, i.e. non-zero value of curl, do not behave like ir-rotational fields which have zero curl. Gravity is zero-curl ir-rotational as are E fields due to charges. Induction E fields are the opposite.

That is my point. Maybe I'm belaboring something not quite within the OP intentions. But several posters stated that an emf exists in free space. I felt compelled to point out that it is a very ambiguous ill-defined non-unique value of emf. In order to have any meaning to the emf concept, a conductor mast be placed in the region and the shape of said conductor determines the emf. Rearranging said conductor shape changes the emf. That is all I wish to emphasize. Sorry if I got carried away. BR.

Claude
 
  • #162
Something we haven't actually stated explicitly in this thread is that the 'EMF' we are discussing is not really a single EMF but a set of EMFs in series, along the coil or around the tube. The line integral is what counts and all the EMFs around the tube go to make up the effective emf which is applied across the resistance of the metal area. So I agree with what you say about the path being important for the final answer. Kirchoff II doesn't translate directly to circuits where 'induction effects' can't be localised to a point in the circuit.
 
  • #163
'A scientist' says that there may be much more water in the Earth's mantel than in all the Oceans.
 
  • #164
cabraham said:
That is my point. Maybe I'm belaboring something not quite within the OP intentions. But several posters stated that an emf exists in free space. I felt compelled to point out that it is a very ambiguous ill-defined non-unique value of emf. In order to have any meaning to the emf concept, a conductor mast be placed in the region and the shape of said conductor determines the emf. Rearranging said conductor shape changes the emf. That is all I wish to emphasize. Sorry if I got carried away. BR.
That's alright. jsmith said he/she? would be away until Sunday anyway. You're right, the closed integral of E*dL does depend on the path. But this doesn't mean it is ill-defined, it just means we must specify the path. If we define the integral of E*dL as the emf, then the emf depends on the path specified (in other words, asking about the emf between two points is useless, unless we also state what path it is taken over). There is no problem with this. It is the more correct way of thinking. When we start talking about a wire, then the path is implied to be through the wire, but if we were speaking more accurately, we would also need to state explicitly what the path is.

I think in an earlier post you said something like 'what use is emf when there are no charges or currents?' And this is a good question. I can't think of any use in classical EM. And I doubt there is any use in EM without charges or currents in general relativity (although I'm not sure, because I don't know a lot about general relativity). This is probably why a lot of people define emf as existing only in a circuit - because there is not much use for the concept when there is no circuits. I would not impose this extra restriction, because I don't like to complicate a definition any more than is necessary, but it just depends on personal preference.
 
  • #165
About this idea of a displacement current which causes a current to flow despite a very large resistance of the oscilloscope: This would mean we are saying the scope effectively acts as a capacitor, right? At first guess, I would have thought that the scope is designed so that it does not act as a capacitor. Also, there is the issue that the induced electric field might not change quickly enough to allow a significant displacement current. Both these issues are difficult to calculate.

I Looked it up on wikipedia, found: "General-purpose oscilloscopes usually present an input impedance of 1 megohm in parallel with a small but known capacitance such as 20 picofarads." So our equation for the current is:
[tex]I = N C \frac{\partial^2 \Phi}{\partial t^2} [/tex]
(where N is the number of turns of the coil, and C is 20 picofarads). So our answer depends on the twice differential (with respect to time) of the magnetic flux. This is a bit more difficult to estimate. We can say we are using a magnetic dipole, which is falling under gravity, and the magnetic flux will be the integral of the magnetic field over the area inside the coil (which will vary at different points in the area, and depend on the distance of the area from the dipole). Difficult :(

Anyway, I should go to bed. I should have been asleep already!
 
  • #166
BruceW said:
When the magnet is in the middle of the coil, you are right that there is zero emf across the entire coil.

When the magnet is above the middle of the coil, the current will flow anticlockwise. This movement of charge will decrease the rate of change of flux below the magnet, but will increase the rate of change of flux above the magnet. But because the magnet is nearer the top half of the coil, the effect of the current flowing above the magnet is less than the effect of the current flowing below the magnet, so overall the rate of change of flux is decreased.

From this explanation, you can see that the braking effect will be zero when the magnet is in the middle of the coil, since there is as much coil above as there is below, so if there was a current, it would have no effect on the magnet's motion.

back a little early!

(from the oscilliscope we can see the emf is zero for the entire time the magnet is in the coil)

so let's say we connected an ammeter instead of an oscilliscope as a current would definately flow then. you seem to be saying we would only get no breaking effect when the magnet is EXACTLY in the centre of the long coil.
using your logic (when the magnet is above the centre there is a greater change in flux beneath the magnet) there should be an emf.
I think a better way to think of it is the amount of flux linking with the coil. When the entire magnet is inside the coil there is no change of flux linking with the coil so no emf is induced.

Having never performed the experiment with a coil I actually don't know the results but I would presumed, base on my way of thinking we would only get magnetic breaking at the ends of the magnet (i.e: as it enters and as it leaves).

I may be getting terribly confused in which case I apologise.
 
  • #167
jsmith613 said:
I may be getting terribly confused in which case I apologise.
No, you're not confused, you're pretty much right. But the emf would be slightly non-zero when the magnet was in the coil. If you think about it, the graph of emf is smooth, this is because there is still a slight emf even when the magnet has entered the coil.

The other way to think about it, is that when the magnet is inside the coil, there is less flux linkage than if the magnet was right in the middle of the coil, so the flux linkage is still changing even when the magnet is inside.

But I think you are right, that the emf when the magnet is inside the coil is much less than when the magnet is entering/leaving the coil. (Especially if the coil was quite long, the emf would be very small when the magnet was inside).

So for an exam, I would just say there is an emf when the magnet is entering/leaving. (Since the emf when the magnet is inside will be an order of magnitude smaller). I hope I haven't made things unnecessarily confusing.
 
  • #168
BruceW said:
No, you're not confused, you're pretty much right. But the emf would be slightly non-zero when the magnet was in the coil. If you think about it, the graph of emf is smooth, this is because there is still a slight emf even when the magnet has entered the coil.
The emboldened statement does not make sense but the rest of it does

so there will be no magnetic breaking effect (for A-level purposes), right?
thanks :)
 
  • #169
jsmith613 said:
so there will be no magnetic breaking effect (for A-level purposes), right?
thanks :)

That's definitely the right A level answer for the coil.
 
  • #170
sophiecentaur said:
That's definitely the right A level answer for the coil.

cheers
once again I must express my gratitude to EVERYONE who has helped me in this discussion
I do hope that the tangent discussion interested other people as well...you can now discuss to your hearts content :)
 
  • #171
No problem.
The one big risk on this forum is over-answering questions. I'm sure it has given many A level students real headaches. "I only wanted to know . . . . . ."
Even when the questioner states his or her level of interest, that doesn't necessarily deter the enthusiastic contributor.
Good luck with the A level stuff.
 
  • #172
jsmith613 said:
The emboldened statement does not make sense but the rest of it does

so there will be no magnetic breaking effect (for A-level purposes), right?
thanks :)
For A-level purpose, yes, there is only a braking effect when the magnet enters and leaves the coil. I think you've got a pretty good grasp of this stuff. Good luck anyway, even though I don't think you'll need it :)
 
<h2>1. What is electromagnetic induction?</h2><p>Electromagnetic induction is the process of generating an electric current in a conductor by exposing it to a changing magnetic field. This is based on the principle discovered by Michael Faraday in the early 19th century.</p><h2>2. How does induced current and EMF relate to electromagnetic induction?</h2><p>Induced current is the flow of electric charge that is generated in a conductor when it is exposed to a changing magnetic field. This induced current also creates an electromotive force (EMF) which is the potential difference that drives the current flow.</p><h2>3. What factors affect the magnitude of induced current and EMF?</h2><p>The magnitude of induced current and EMF depends on the strength of the magnetic field, the speed at which the magnetic field changes, and the characteristics of the conductor such as its length, shape, and material.</p><h2>4. How is electromagnetic induction used in everyday life?</h2><p>Electromagnetic induction has numerous practical applications, including power generation in generators, transformers, and motors. It is also used in devices such as induction cooktops, wireless chargers, and metal detectors.</p><h2>5. What is the difference between AC and DC current in terms of electromagnetic induction?</h2><p>AC (alternating current) is the type of current produced in a generator through electromagnetic induction, where the direction of the current changes periodically. DC (direct current) is a constant flow of current in one direction, and it is typically produced by batteries rather than through electromagnetic induction.</p>

1. What is electromagnetic induction?

Electromagnetic induction is the process of generating an electric current in a conductor by exposing it to a changing magnetic field. This is based on the principle discovered by Michael Faraday in the early 19th century.

2. How does induced current and EMF relate to electromagnetic induction?

Induced current is the flow of electric charge that is generated in a conductor when it is exposed to a changing magnetic field. This induced current also creates an electromotive force (EMF) which is the potential difference that drives the current flow.

3. What factors affect the magnitude of induced current and EMF?

The magnitude of induced current and EMF depends on the strength of the magnetic field, the speed at which the magnetic field changes, and the characteristics of the conductor such as its length, shape, and material.

4. How is electromagnetic induction used in everyday life?

Electromagnetic induction has numerous practical applications, including power generation in generators, transformers, and motors. It is also used in devices such as induction cooktops, wireless chargers, and metal detectors.

5. What is the difference between AC and DC current in terms of electromagnetic induction?

AC (alternating current) is the type of current produced in a generator through electromagnetic induction, where the direction of the current changes periodically. DC (direct current) is a constant flow of current in one direction, and it is typically produced by batteries rather than through electromagnetic induction.

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