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A paradox about Drift Velocityby newtonrulez
Tags: drift speed 
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#19
Feb1810, 05:50 PM

P: 262

In my example the force is 17KN and the area is 4X108 m2 so that the pressure is F/A=4x10^11Pa. Now whether there’s one particle or 10^11 particles is for this calculation immaterial. The small copper wire has to deal with this pressure! To mehslep: You are correct about the power losses. But keep in mind that those electrons also have to transport power to the point where its needed. How in your opinion does the power reach its destination far away from the source? (Remember we're still dealing with the stick/sweetie/water analogy) 


#20
Feb1810, 07:06 PM

PF Gold
P: 3,098




#21
Feb1910, 05:35 AM

P: 262

So it looks like indeed many generations of students have been taught the wrong concept. Its impossible to transport any kind of everyday meaningful amount of power using such a low velocity. The stick theory just doesn’t work. How many physics books are still going to be written with this wrong concept? We could go into how the electromagnetic field does the work but that is too far away from the OP and could do with a new post. 


#22
Feb1910, 06:05 AM

PF Gold
P: 2,020

P=N times Fv N= number of electrons in wire F=force acting on each electron=electron charge * electric field strength Because N is large the power is large.Please note that A cancels and that the force originally calculated would be the force if the power was carried by one electron only. 


#23
Feb1910, 03:12 PM

P: 262




#24
Feb1910, 03:47 PM

PF Gold
P: 2,020

I=nAve..........................................1. P=VI..............................................2. n=no of free electrons/unit volume=N/Al Substituting and tidying up we can write: P=N*Ve/l*v=N*F*v 


#25
Feb2010, 05:50 AM

P: 262

First we have to define what the “stick” theory means. It means the transport of power from source to load in a longitudinal (length way) manner. Much like when, holding a stick, you can push and pull a heavy stone across a rough surface. This way of power transport is similar to hydraulic, water, chain, etc in fact any mechanical way of power transport. Do you go along with that explanation? Then my claim is that to have any meaning full transport of power this way we need some kind of reasonable speed of medium otherwise forces and pressures become too high for any everyday material (and size) let alone soft copper. 


#26
Feb2010, 07:11 AM

Mentor
P: 17,220

Per Oni, your calculation of the stress in a current carrying wire is WAY off. The stress due to an arbitrary EM field is given by the Maxwell stress tensor which is:
[tex]\sigma _{ij} = \varepsilon_0 E_i E_j + \frac{1} {{\mu _0 }}B_i B_j  \frac{1}{2}\bigl( {\varepsilon_0 E^2 + \tfrac{1} {{\mu _0 }}B^2 } \bigr)\delta _{ij} [/tex] For a typical maximum 15 A circuit on 14 gauge copper wire used in home wiring the diameter is about 1.6 mm and the resistivity is 1.72E8 Ohm m. The magnetic field due to a long isolated current carrying wire is perpendicular to the wire (right hand rule) and of magnitude: [tex]B=\frac{\mu_0 I}{2 \pi r}=0.00375 \: T[/tex] The electric field in a resistive wire is parallel to the wire and is of magnitude: [tex]E=\rho J = 0.128 \: V/m[/tex] For the tensile stress on an isolated current carrying wire on the z axis you would be interested in the z,z component of the stress tensor. [tex]\sigma _{zz} = \varepsilon_0 E_z E_z + \frac{1} {{\mu _0 }}B_z B_z  \frac{1}{2}\bigl( {\varepsilon_0 E^2 + \tfrac{1} {{\mu _0 }}B^2 } \bigr)\delta _{zz} = 5.60 \: Pa[/tex] Which is more than 10 million times smaller than copper's yield stress of 70 MPa. To get the kinds of stress you are imagining would require something on the order of 4 MA. Yes, 4 MA will indeed destroy 14 gauge copper wire. In any case, the density of the charge carriers can be easily measured with the Hall effect. Once the density of charge carriers is known then there is no ambiguity whatsoever about the drift velocity for a given current density. The density of charge carriers is enormous, leading to very slow drift velocities. 


#27
Feb2110, 07:55 AM

P: 262

I will have a closer look at your calculations when I've got some time. In the mean time thanks for taking part. 


#28
Feb2110, 09:57 AM

P: 262

Dalespam:
I’ll try to explain as carefully as pos what my objections to this thread are, not that I want to talk down to anybody but I am plainly bad at explaining myself. The suggestion in this thread is that the signal speed of current in a wire can be explained using the analogy of a tube of sweeties where one enters, side pushes all the adjacent sweeties so that the last one pops out of the tube at the far end. This picture is wrong for a number of reasons. I wanted to show what the implications are, considering the forces involved transporting any average power that way, knowing that the medium (sweeties) travel at an extremely slow speed. Because that way since F=P/v, force and therefore pressure become very high indeed. A second objection is that it doesn’t even explain the electrical signal speed. Use the analogy of say a metal bar. When we push this bar a small distance length ways the pressure wave travels at approx the speed of sound for that metal, far short of the signal speed which is close to the speed of light. There are more points but I hope you get why I objected. As for your solution, mheslep and I already indicated that electromagnetic theory can explain the ins and outs. I am a little puzzled why you reacted to my correct post and not to some of the previous wrong posts. 


#29
Feb2110, 10:41 AM

PF Gold
P: 2,020

Hello Per Oni.I think all analogies have their weaknesses and shortcomings and you have pointed out some of these with the stick and sweeties analogies.Despite these weaknesses these analogies can be useful provided they are presented with care.I suppose it could be argued that free electron theory is itself an analogy.



#30
Feb2110, 01:30 PM

PF Gold
P: 3,098




#31
Feb2110, 01:39 PM

PF Gold
P: 2,020




#32
Feb2110, 03:13 PM

P: 262

However now use sweeties / ball bearings etc. in a tube instead of electrons and you will find that for 100W to be supplied with v= 0.006 m/s there’s a big force present on this medium. I suppose the real difference is that electrons carry (are carriers of) electro magnetic fields. Any disturbance in these fields are propagated close to the speed of light, depending on what kind of cable and insulation. 


#33
Feb2110, 05:15 PM

Mentor
P: 17,220

Also, the analogy is not so far from the truth. When you push one sweetie in on one end one pops out on the other end (conservation of charge). Moving the sweeties heats up the tube (resistance) and reduces the force that the last sweetie can push with (voltage drop). The last sweetie doesn't quite start moving instantaneously (finite speed of light). Etc. As with all analogies it fails at some point, and it is good to point that out to students. In this case it fails to explain the stress of the EM field. But if we were to insist that all analogies be completely perfect in all situations then we could never use any analogies at all. The analogy is good (although I prefer the plumbing analogy to the sweeties one) and is useful to students in learning a challenging subject. It correctly addresses the OP's question which did not extend to EM stress or other topics outside of the proper scope of the analogy. 


#34
Feb2210, 04:17 AM

P: 262

As to your feeling that the plumbing theory it is sort of ok, some time ago I read an article (it could be wiki) which proposed 2 different theory’s of electrical conduction one based on plumbing and one following the theory of the Poynting vector. (Perhaps it has been removed?) If we don’t point out discrepancies eventually it will end up all the way up there. Just reading some wiki pages I found this: http://en.wikipedia.org/wiki/Poynting_vector: There’s another aspect of electrical conduction theory I like to mention, namely: energy leaves the source at near light speed towards the surrounding dielectric. Therefore it follows that the source should receive a kickback in the opposite direction. Has anyone ever seen a paper dealing with that fact, or anyone any thoughts? 


#35
Mar110, 05:04 PM

P: 8

Here is the simple explanation. The switchon time is not dependent on the drift velocity. After the circuit is switched on, the electric field is applied on the appliance immediately (the speed of the propagation of the field is about 1/10 of the speed of light). At the same time the electrons start to drift and thus current is formed. We can also say within the time of the length of the circuit divided by 1/10 of the speed of light, the drift velocity along the wire can reach the same value. The time that is consumed is not dependent on the drift velocity but the speed of the propagation of the electric field.



#36
Mar810, 07:28 PM

P: 152

To get an approximate idea of the order of drift velocity without much math,
charge of electron is roughly 10^19C, so a one amp current in a wire corresponds to an exchange of 10^19 electrons per second, since these are the charge carriers. A piece of matter that you hold in your hand has roughly 10^23 atoms, (via avogradro). so you figure you have roughly 10^23 valence electrons (via atoms), but you only need to move 10^19 of them every second. So they must move on average 10^4 m/s. Quick approximation, you'll do better by knowing the current, current density, & concentration of valance electrons. Specifically, the drift velocity doesn't mean thats how fast the signal propagates. If I move an electron on one side of the wire, that coulomb field (disturbance) propagates at the speed of light. In practice the electron at one end of a wire never reaches the other end (according to this classical drift velocity idea), it would take an awfully long time. However the signal particularly in Ac propagates at "near" (see last line) the speed of light. Even with :slowed: light in a medium, the light still travels at C, its just the light gets absorbed and re emitted and this takes a certain amount of time which delays the light. the light however always travels at C, but we speak of the speed of the light in the medium to include these absorption and emission times. Another thing to keep in mind, the coulomb disturbance mentioned above is mediated by light itself, so it will feel the effects of the delay time, all relative to permittivity and permeability. 


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