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Can a magnetic fields/forces do work on a current carrying wire?! |
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| Jul26-12, 08:06 AM | #120 |
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Can a magnetic fields/forces do work on a current carrying wire?!1) Let's use the definition of work as energy transfered to or from a system by any mechanism other than heat. 2) Only external forces can do work on a system since internal forces cannot transfer energy in or out of the system. 3) A system's KE may change without work being done on the system, provided there is some compensatory change in some other form of energy for the system. (this is what I neglected in my example) 4) If the paper represents some specific examples of a general principle, then in all situations where the magnetic force is the only external force, any change in KE must be accompanied by a corresponding change in some other internal form of energy. So, in my example, an external magnetic field can accelerate (increase KE) a superconducting loop. This must be accompanied by a decrease in internal energy. The only available energy is the energy density of the magnetic field, which depends only on the current. Therefore, the current in the loop must decrease as the loop accelerates. Although I didn't calculate it explicitly, this makes sense to me. A motor is easy to explain since the magnetic field is not the only source of energy transfer. However, the one thing that makes me hesitate to adopt this principle wholeheartedly is that it is not always clear what internal energy is being used. For example, consider a permanent magnet being accelerated in an external magnetic field. What is the internal energy that is being used in the permanent magnet? Any ideas? |
| Jul26-12, 09:20 AM | #121 |
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Work done on charges according to this dot product is that of the E field along the direction of charge motion. We know that J = sigma*E, so that J & E are generally in the same direction. J dot with E is simply sigma*E2. But this work being done on the charges is that of conduction current. The current in the loop consists of charges acted upon by E force so that the current density J is along the direction of E force per Lorentz law. We already knew that. Again, let us convey an example. An induction motor is a good case to examine. The stator is connected to an ac power source, constant voltage, 60 Hz, etc. A rotating field is established. Current in the stator results in a mag field which revolves about the stator axis linking the rotor bars, for a squirrel cage type rotor. This rotating B field is accompanied by a rotating E field. The current induced into the rotor consists of charges acted upon by Lorentz force. What force is doing the work of moving e- around the rotor loops resulting in a rotor generated revolving magnetic field? The only answer is the E force. The equation you gave is applicable here. The B force acts radially to the rotor bar electrons, E force moves them around the loop. I doubt that anyone here would dispute that the rotor charges moving in the rotor loop are motivated by the revolving E force, not the B force. Hence the work done on the rotor charges moving in the rotor loop is done by E force. Pretty obvious. But now that rotor current is realized, a revolving rotor magnetic field exists. This field interacts with the stator field & a torque is produced. As the rotor is moved towards the stator, energy is expended, & the mag field must be replenished. The ac power mains source does just that. Your integral shown above relates the work done on charges to the dot product of E & J. Draw a diagram & it is plain as day that that is the work establishing rotor current, not the work done turning the rotor through an angle. E is in the direction of J, if E is normal to J, dot product goes to 0. The force on the rotor is not along the direction of J. It is normal to J. The "E dot J" in your integral is not what you think it is. I will accept correction if I erred, but please give us references as to the orientation of B force, E force, J, etc. Thanks for your interest. Claude |
| Jul26-12, 09:21 AM | #122 |
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[tex]\vec{j}=c \vec{\nabla} \times \vec{M}.[/tex] Now, the permanent magnet is accelerated by the external magnetic field and according to Faraday's Law this induces an electric field which in turn leads to a current counteracting the change (Lenz's Rule). So again you have an change of intrinsic energy, and the work done is solely due to the induced electric field as it must be according to Poynting's Theorem! |
| Jul26-12, 09:32 AM | #123 |
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| Jul26-12, 09:56 AM | #124 |
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The induced current is a usual conduction current (caused by the conduction electron's motion in your metal permanent magnet). There's nothing exotic in this.
There's a lot of confusion on this issue, because many textbooks still use the pretty vague ideas of 19th century electromagnetism, where the inner structure of matter hasn't been as well understood as nowadays. The best introductory book about a more modern point of view on "macroscopic electrodynamics" is vol. II of the Feynman Lectures. In fact it has been 19th century electromagnetism that paved the way to gain this understanding. A first highlight was the development of (special) relativity (which you can still count as 19th-century physics although it was finished only 1905 with Einstein's famous paper and the 1907 paper by Minkowski on covariant macroscopic electromagnetics). Another one the development of "classical electron theory" by Lorentz, Abraham, et al. Finally the many contradictions and problems in the description of atoms lead to the main achievement of 20th century physics, namely quantum theory, which again was triggered by a purely electromagnetic problem, namely the problem of the spectrum of thermal radiation, which lead to the discovery of the "action quantum" [itex]\hbar[/itex] by Max Planck in 1900 and the development of "old quantum" theory, again by Einstein with his "heuristic point of view" of electromagnetic radiation as light corpuscles (1905) and Bohr's and Sommerfeld's quantum model of the atom (again a work on electromagnetism, namely the motion of electrons around a nucleus, 1912-1916). Finally it lead to the development of modern quantum mechanics (Heisenberg, Born, Jordan, Pauli; Dirac; Schrödinger 1925-1927) and quantum electrodynamics and finally relativistic quantum field theory. BTW: Physicswise we still live in the 20th century, because there's no new big paradigm change at the horizon yet. To the contrary: The preliminary discovery of hints for a (quite boring form of a minimal standard-model) Higgs again confirms the good old Standard Model of elementary particle physics :-(. |
| Jul26-12, 10:22 AM | #125 |
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However, then suppose the magnet transitions to a region with a uniform field. At this point there is no more flux and therefore no more induced current. The magnet's internal field is no longer partially canceled so its internal energy returns to normal, but it still has KE. I think the change in energy must be more than just a conduction current in this case. I am just not sure what else it could be. |
| Jul26-12, 11:00 AM | #126 |
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Another thing to consider is that in the situation where the wires are held stationary and we only have magnetic forces, from the rest frame of the charges in the wires there only exists an electric field. This is a common problem that is worked in texts like Griffiths. So from the electron's point of view, it only sees an electric field and not the magnetic field. In that case why not conclude that it is still the electric field that does all the work? So the take away point that I would make is that with the wires, we need to keep in mind that it isn't an electric or magnetic field but an electromagnetic field. You can't conclude that the magnetic fields do the work from the face of it. |
| Jul26-12, 11:22 AM | #127 |
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2nd bold: "From the electron's point of view ---". We understand that when we view a motor spinning, we are viewing it from our static reference frame. We have already conceded that a free e- in conduction cannot have work done upon it by a B force, only an E force. You keep rehashing isolated particle physics & emphasize facts I've already conceded to. Nobody is disputing that. Also, the electron sees a static E field from the other loop's stationary lattice protons. But it sees a B field due to the other loop's electrons in motion. The electrons moving in the other loop undergo a Lorentz-Fitzgerald contraction, so that mere E force is not adequate to explain the force here. 3rd bold: "we need to keep in mind that it isn't an electric or magnetic field but an electromagnetic field". What on earth is an "electromagnetic field"? Please enlighten me. There are magnetic quantities B & H, electric quantities E & D. Just how do you describe this "electromagnetic field"? Please enlighten me. So far the naysayers have produced nothing. They talk a big game about Einstein, reference frames, etc., but cannot show me the fields working in a simple induction motor. Show me, please, how it is E force, & not B force that spins the rotor. So far all I get is people blowing smoke. Not 1 naysayer has addressed the motor operation question. In a motor, we are not simply moving electrons from valence to conduction. We are exerting forces on wire loops resulting in torque & work being done. Making a loop spin involves more than conduction current. A B force acting on free electrons in a loop producing torque is more involved than simply inducing a loop current. The B force yanks on the e-, but the p+ & n0 get tethered as well. These e-, p+, & n0, all moving together in unison constitute zero current. Of course the current in the rotor loop is non-zero. There is more than 1 thing going on here. Claude |
| Jul26-12, 01:28 PM | #128 |
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| Jul26-12, 02:56 PM | #129 |
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| Jul26-12, 10:38 PM | #130 |
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"Not 1 naysayer has addressed the motor operation question." THANK YOU! I really like were you're going with this Claude + Agree with you're argument all the way! Magnetic forces generated on the current loop/stator etc... Is all due to the magnetic field! THE MAGNETIC FIELD CAUSES THE ROTATION and WORK TO BE DONE!(Not it alone by has a primary key role in this whole process). Many keep denying that fact WHY?! What give you that idea? Even when you deny it you'd refere to a single charge... Well read the thread topic... Were talking about the effect thats present within a motor! Why include that law that is irrelevant to it? That law is based on "A" charge... Please state you're opinion or idea based on the "motor effect". Not one the quantum scale of things where everything's different. |
| Jul27-12, 07:51 AM | #131 |
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http://en.wikipedia.org/wiki/Covaria...ectromagnetism With this formulation the separation of the EM field tensor into an E field and a B field is seen as a simple artifact of the coordinate system chosen. Since the choice of coordinate system is arbitrary, so is the distinction between E and B. Regarding naysayers, I haven't yet made up my mind. I came into the thread quite convinced that magnetic fields do work, but I am no longer so certain after having read the paper referenced above. Did you read it? If so, did you find any specific errors? However, the reason that I used a superconducting loop in my example rather than a motor is the obvious weakness of the motor argument: specifically, the motor has a large amount of E field energy going into the system on the wires. I wanted a "cleaner" system where the only possible work was done by the B field, which is not the case with a motor. |
| Jul27-12, 08:45 AM | #132 |
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Now when it comes to moving e- through the loop, work is needed. As electrons collide with the lattice, losing energy & radiating photonic emission (heat which is I2R), they need to have work done on them to replenish said energy. This work is done by E, not by B. Thus the work done on the charges in the loop(s) maintaining the current, is done only by E, not by B force. Fair enough? Claude |
| Jul27-12, 09:12 AM | #133 |
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| Jul27-12, 09:34 AM | #134 |
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Claude |
| Jul27-12, 09:49 AM | #135 |
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Btw, did you read the paper? What did you think? |
| Jul27-12, 10:44 AM | #136 |
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The wiki link gives a good primer as to how special relativity relates to e/m field theory. Both references are very useful & well written. But we already have many text books written on motor operation. Do we really need to examine the OP question from the viewpoint of reference frame other than a stationary observer watching the motor spin? We seem to have gone off on a tangent. This weekend I will create a sketch & post it. Based on Ampere's Law, Faraday's Law, the magnetic vector potential A, E field, B/H field, etc., the only logical conclusion is that to turn the rotor, a force must exert a torque on said rotor. Only B/H seems to have the correct direction to do that. E acts tangential to the loop. resulting in induced current as Lorentz force describes. To get a torque you need a B force. But to have a B force you need 2 currents. Each current is established & maintained by E forces. But those E forces rely on B fields as well. The E field in the rotor maintains rotor current. But the rotor E is due to the stator B field. Stator B is due to stator I, which is related to stator E. I think I'm on solid ground when I say that E, B, V, I, torque, & speed are very interactive. No single entity is responsible for motor action. But B produces the torque. But w/o E, I, V, etc., there wouldn't be any B. Likewise B only yanks on electrons, then the protons & neutrons are tethered via E & SN forces. B cannot do it alone. That has been my position w/o wavering. Claude |
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