So far, we have only discussed in this course,
electricity. Calm down. But this course is about electricity and magnetism. Today, I'm going to talk about magnetism. In the fifth century B.C., the Greeks already knew that there are
some rocks that attract bits of iron. And they are very plentiful in the district
of Magnesia, and so that's where the name "magnet" and "magnetism" comes from. The rocks contain iron oxide, which we will
call, uh, magnetite. In eleven hundred A.D., the Chinese used these needles of magnetite
to make compasses, and in the thirteenth century, it was discovered that magnetites have two
places of maximum attraction, which we call poles. So if you take one piece of magnetite, it
always has two poles. Let's call one pole A, and the other B. A and A repel each other, B and B repel each
other, but A and B attract each other. There is a huge difference between electricity
and magnetism. With electricity, you also have two polarities, but you are free to choose a plus or a minus poles With magnetism, you don't have that choice. The poles will always come in pairs. Isolated magnetic poles do not exist -- or,
as a physicist would say, magnetic monopoles do not exist, as far as we know. If anyone finds a magnetic monopole -- and
don't think that people are not looking -- that would certainly be worth a Nobel Prize. In principle, they could exist, but as far
as we know, they don't exist, they have never been seen. Electric monopoles do exist. If you have a plus charge, that's an electric
monopole. You have a minus charge, electric charge,
that is an electric monopole. If you have a plus and a minus of equal strength,
that is an electric dipole. Whenever you have a magnet, you always have
a magnetic dipole. There is no such thing as a magnetic monopole. In the sixteenth century, Gilbert discovered
that the Earth is really a giant magnet, and he experimented with compasses, and he was,
effectively, the first person to map out the elec- the magnetic field of the Earth. And if you take one of those magnetite needles,
and the needle is pointing in this direction, which is the direction of Northern Canada, then, by convention, we call
this side of the needle North and we call this side
of the needle south. Since A repels A, and B repels B, but A and
B attract each other, in north Canada is the magnetic South Pole of the Earth,
not the magnetic North Pole. That's a detail, now, of course. So this is the way that we define the direction,
north and south, of these magnetite needles. A crucial discovery was made in eighteen nineteen
by the Danish physicist Oersted. And he discovered that a magnetic needle responds
to a current in a wire. And this linked magnetism with electricity. And this is arguably, perhaps, the most important
experiment ever done. Oersted concluded that the current in the
wire produces a magnetic field, and that the magnetic needle moves in response to that
magnetic field which is produced by the wire. And this magnificent discovery caused an explosion
of activity in the nineteenth century -- notably by Ampere, by Faraday, and by Henry -- and it culminated into
the brilliant work of the Scottish theoretician Maxwell. Maxwell composed a Unified Field Theory,
which connects electricity with magnetism. And that is at the heart of this course. Maxwell's equations. You will see them, all fear -- all four, by
the end of this course. If I have a current, a wire, let's say the
wire is perpendicular to the blackboard, and the current goes into the blackboard, I put
a cross in there. If the current comes out of the blackboard,
I put a dot there. And there is a historical reason for that. You're always talked about vectors,
in 18.01, and in other courses, but you're never
seen a vector And I'm going to show you a vector. This is a vector. And this is when it comes to you. That's when you see a dot. And this is where it goes away from you. That's when you see a cross. So this current, when it's going into the
blackboard, I can put these magnetite needles in its vicinity, and they will then do this. And when I put it here, it will go like this. And they follow a circle,
and this the way that we define magnetic fields, and the direction of the magnetic
field, namely, that the magnetic field -- for which we always write the symbol B, magnetic
fields -- is now in the clockwise direction. By convention, current goes into the blackboard. And, if you ever forget that, use what we
call the right-hand corkscrew rule. If you take a corkscrew, and you turn it clockwise,
the corkscrew goes in the board. That connects the B with the current. If you take a corkscrew and you rotate it
counterclockwise, then the corkscrew would come to you, comes out of the cork. And that's how you find the magnetic field
going around current wires. It's just a convention. I want to show you how a magnetic
needle responds to a current. I have here a wire through which I'm going
to run a fabulous amount of current, something like three hundred amperes, and you're going
to see that wire there I'm going to get my lights right, see how I want it to go,
this is the way I want it to go, get you optimum light there. When I draw a current -- here, you see the
the magnetite, the -- we call it a compass nowadays -- and it's lined up in the direction
of the magnetic fields of the Earth. We're going to run three hundred amperes through
here, and it will change the direction, it will change the direction which is -- there's going to be a magnetic field
around the wire -- like this. So it will go like this. The current that I run is so high that things
begin to smell and smoke within seconds. The battery is not going to like it when I
draw such a high current. I can, therefore, do it only for a few seconds. So this compass will swing in this direction,
and it starts to oscillate, I can't keep the current so long
that it stops the oscillation. So I will stop it by hand, and convince you
that that's really the equilibrium position. So if you're ready for that --
so we get, now, connection, watch it three, two, one, zero There it goes. And I'll stop it -- the current is still going. You see, that's the -- that is the equilibrium
position. And I will stop the current. And now I will reverse the current, in the
opposite direction and now you will see that it swings backwards. It -- hundred and eighty degrees in a different
direction. Three, two, one, zero. There it goes, I will stop it, [sniffs], few
seconds, that's the equilibrium position, and I'll let it go. So you've seen that, indeed, the magnetic
needle responded to the magnetic field that was produced by the wire, this was the great
discovery by Oersted, the discovery this demonstration, all by itself, may not be very
spectacular for you, but, historically, it is of enormous importance. I would argue, perhaps, the most important
demonstration, the most important research ever done in physics, because it connects
electricity with magnetism. It was the foundation of the creation of the
whole concept of a field theory. Action equals minus reaction, and that
means that if a wire that runs a current has a force on a magnet, then, of course, the
magnet must also exert a force on the wire. And I'm going to demonstrate that to you,
too, but now, I have a much more potent magnet, for which I will use this one, and the magnet
will not move, it's so heavy that it can't move so now you will only see the wire
move. And the basic idea is then as follows, here
is that magnet. This is the north pole of the magnet,
and this is the south pole. I don't remember which is which,
to be frank with you -- so the magnetic field would run, then, like so, and I have, here,
a current wire, a wire that runs a current through it. The wire is perpendicular to
the blackboard. If, when I turn the current on, if the current
is coming out of the blackboard -- and I have fifty percent chance, because I really don't
remember whether this is north or south -- but let's assume that this is the configuration,
that the current is coming out of the blackboard, then you will see this wire
experience a force up. It is an experimental fact that the force
on the wire is always in the direction of I cross B. These are unit vectors. And since I is coming
out of the blackboard, if I cross I with B, I get a
force in this direction. And so if I reverse, now, the current -- if
the current goes like this, then, of course, the wire
wants to go down. And I will show you both. But I don't know which one will come first,
because I didn't mark the poles. Ahh -- uhh. So you see it, now, slightly different from
the way I have drawn it. I've drawn you the magnet
looking this way, but it's, of course, much nicer
for you to see it this way So you see the wire, and there is the magnet,
and now I'm going to run a few hundred amperes through that wire, and then it either will
jump up, or it will jump down, and then I will reverse the current,
and then the opposite thing will happen. OK. We ready for this? Three, two, one, zero. Notice, there was a distinct force down, the force was so high that
it even pulled down the supports So now I can predict that if I reverse the
current from this experiment, that now the wire will jump up. There we go -- I know now, exactly, because
I switched it this way, so now I will switch it this way, and the wire will jump up. That's the first drawing you see. Three, two, one, zero. Very clear. You saw it come out. OK. Let me take this down. All right. If I have a wire, through which I run a
current let's say I run a current I1
through this wire it will produce a
magnetic field, right-hand corkscrew, right here, that magnetic field will
be in the blackboard I'll call it B1 right here, it will be out
of the blackboard But that's irrelevant right now. But it is out of the blackboard. Here, it's in the blackboard. And here, I have another wire, I'm going to
run a current I2. There will be a force now, on this wire, in
the direction I cross B. Take your hands, I cross B [krrk], that force
is up. So this wire will experience a force up. But of course, if this wire experiences a
force up, since action equals minus reaction, this wire will experience a force down. So they will go towards each other. They will be attracted by each other. You can in an independent way confirm that
the force here is down. So this is the force. For me, it would be enough to say action equals
minus reaction, Newton's Third Law. But if you want to put in here, the magnetic
field B2, which is the result of this current, which is, of course, out of the blackboard,
remember the right-hand corkscrew rule then you will see that this force, now,
here, must be in the direction of I1, crossed with B2. And that's down, which is exactly what I predicted. So the two wires will go towards each other. However, if I leave everything the same, but
I reverse the direction of I2 so now the two currents
are in opposite direction then the forces will flip over, and so now the two wires repel each other. And I will demonstrate that to you. I have those those two wires here, and you will
see them there on the screen. I will explain what you're
looking at in some detail. The two wires run vertically,
this is one wire, and this is the other wire and when I run a current
in the same direction, then they will attract each other. And you will see that shortly. Three, two, one, zero. See? They go towards each other. I will do it again, now. If I run the current in opposite directions,
they will repel each other. Now I run them in opposite directions. They repel each other. I'll do it again, three, two, one, zero. They repel each other. The reason why I showed you this demonstration
is a different one. What I want you to appreciate that if I have
this conducting plate of aluminum, it's a conductor -- and I put that in between the
two wires, and I repeat the experiment, that exactly the same thing will happen. And that tells you that magnetic fields are
really very different from electric fields, because electric fields would be heavily affected
by a conducting sheet like this. Magnetic fields are not. So what I'm going to do now is
I'm going to put this plate in between, and then I'm going to again, put the currents in opposite directions,
and so we will see the wires repel each other as if the plate were not there. Three, two, one, zero. There you go. So magnetic fields have a very interesting
story to tell. However, electricity and magnetism are connected. How do we define the strength
of a magnetic field? With electricity, we defined the strengths of electric fields in the following way, we measured the force,
the electric force, on a charge, on an electric charge, and then the electric force is the
charge times the electric field. That determines the strength
of the electric field. Wouldn't it be nice if we could now say, "OK,
the magnetic force is a magnetic charge times the B field. So that would then define the magnitude of
the B field. That would be nice. But as long as we haven't found a magnetic
monopole, we can't do it. If you come with a magnetic monopole tomorrow,
I can do this. But we have no magnetic monopoles, and so
it cannot be done this way. How is magnetic field then defined? Well,
it is defined in the following way. I take an electric charge, and the electric
charge is q. And if that electric charge moves with a velocity
V, and there is a magnetic field where the electric charge is moving, then it is an experimental
fact that the force is always perpendicular to V. If you want to call that B, with a magnetic
indication, that's fine. So there is a magnetic field, the charge is
moving with this velocity, and there is a force on that charge which is
always perpendicular to V. The magnitude of that force is proportional
to the speed of the particle, and it is also proportional to the charge itself. If I double the charge, then the force doubles. If I double the speed, then the force doubles. And so the way that we define, now, magnetic
field strength, is this way. The force -- and I give it a B to remind you
-- magnetic, is q, is the electric charge, v is the velocity of the electric charge,
the cross-product with B. And you see that the force is always perpendicular
to v, and that it is linearly proportional with the speed, and linearly proportional
with the charge q. And this is often called the Lorenz force
after the Dutch physicist. This equation is completely sign-sensitive. If you change from a positive charge to a
negative charge, then the force flips over, a hundred eighty degrees. You change the direction of v,
force flips over. Change the direction of B, force flips over. So it's a completely sign-sensitive equation. The unit for magnetic field strength follows
from this equation, this is Newton's, q is Coulombs, and v is meters per second. So this would be the unit for magnetic field
strength, but no one would ever say that. In SI units -- this would be SI units -- we
call that one Tesla, for which we write one capital T. A Tesla is an extremely strong magnetic field. The magnetic field of this magnet is only
two-tenths of a Tesla. And that's a very strong magnet. We often use, therefore, a unit, which is
the gauss, which is not an SI unit, but you will see it often in books, and one gauss
is ten to the minus four Tesla. The Earth's magnetic field is roughly half
a gauss. And so this magnet is about two kilogauss. But the SI unit is Tesla. If you had looked at a television in 2002,
when I gave these lectures, or the screen of your computer,
you have a fluorescent screen and in a television, there are electron
guns that raster scan this fluorescent screen on a television screen, you have five hundred
and twenty five lines, and the electron guns scan that it one-thirtieth of a second. And the intensity changes of these electron
beams create images. So if you look at the tube from the side,
then there are electrons one moment in time, they may move like this, another moment,
they may be here, in the raster scan and so it's clear that if you bring a strong magnet
in the vicinity of your television screen, that you will distort the image, because you
are now affecting the motion of these currents, of these electrons. And there is a very famous artist, Nam June
Paik who used this for his art, and almost every major museum in this world has a work by Nam June Paik, with distorted images using magnets and using television screens. I don't want to compete with Nam June Paik,
but I do want to show this to you. I have there, a television set, and I have
a very strong magnet, and I will try to distort that image and give you the best lights that
we know how to. And I suggest we try to find
a program that we hate. So here is my magnet -- oh, man -- this is
an extremely strong magnet, and let's turn on the television, and let's see what we can
get first. Oh, I turned it off instead of on. (tv channels changing) TV: I con't think LEWIN: neither do I (tv channels changing) Ah, I hate commercials.
Let's go for a commercial. Ah I hate commercials,
now, watch it closely Here comes my magnet, there's the image. You see that? Don't do this to your own computer Because once you have done this it may never look the same. but these electrons now. Can you see it? Do you see the distortion? Can you see the distortion? You are so quiet, ok. So you have seen that so you have seen that we can,
with a magnet and a moving charge that we can change the direction of the moving
charge. Force on the moving charges. If you have an electric field as well as a
magnetic field, then, of course, you have also the electric force. And so the total force on a moving charged
particle would then be q times the electric q times the electric field vector,
plus v cross B. And this, of course, we've seen before. An electric field can do work on a charge. Remember, q delta v. Can be positive, can be negative, but it can
do work. It can change the kinetic energy of the charge. Magnetic fields can never do work on a moving
charge. And the reason is that the force is always
perpendicular to the velocity v. And so if the force is always perpendicular
to the motion, you can change the direction of the motion, but you
can't change the kinetic energy. So that's a fundamental difference between
the electric force and the magnetic force. So now I want to calculate, with you, the
force on a current that runs a wire I through it, and we have a magnetic field B. So we're going to be slowly -- we're going
to be more and more quantitative. This, by the way, is often also called
the Lorenz force, just a combination of the two. That one certainly is. So let is start with a wire, and the wire that runs a current through, here is the wire, and the current is I. And let's say, at this point here, we have
a magnetic field B. And the magnetic field could be different
along the wire, in principle. Here, I have a charge, plus dq, and this charge is running through
the wire with a drift velocity v d. Let's first think about what happens if the
current is zero. If the current is zero, at room temperature,
these free electrons in these wires have huge speeds. Three million meters per second. Way larger than the drift velocity. But they are in all chaotic directions. Random motion, it's a thermal motion. And so on each individual charge, there will
be a force. But they average out to be zero. It's not until I run a current that these
charges are going to walk through with a very slow drift velocity, and now, of course, the
net force is not zero. So let's have this charge dq that moves in
this direction, and so that gives me a current. And let this angle be theta between them. Say, that's going to be important, because
it's a cross-product between velocity and B. That means the sine of
this theta comes in later. You will say -- I hope you will say, "Well,
listen, man, this is ridiculous. Uh, positive charges don't move through wires. It is the electrons that move through wires. They are responsible for the current. And electrons have a negative charge, and
they go in this direction. You're right. Perfectly fine. However, a negative charge going in this direction
is mathematically exactly the same as a positive charge going in that direction. In both cases, do we agree that the current
is in this direction. So I have preferred, for mathematical reasons,
to take a plus dq charge going in this direction rather than taking a minus dq charge that
goes with the drift velocity in that direction. So there is no difference at all in the outcome
that you will see. So on this charge, there is a force, dF it is this magnetic force, and that is the charge dq,
that equation, times v cross B. Well, v was that drift velocity, and here
is the magnetic field, at this location. The current through the wire, everywhere on
the wire, must be dq / dt. Because that's the definition of current,
how many Coulombs per second. Current is always dq / dt. So I can also write this as I dt
times vd cross B. But I remember 8.01, that vd times
dt, that is speed times a time is a distance. And I call that distance dl. It's a distance along the wire. I will put a distance in here now, because
I don't want to clutter up my -- my drawing. So this charge, in time dt, moves over that
distance, that's a vector. 8.01. So I can write down for this product, I can
write down dl. So I can also write down that dF of B equals
I times dl cross B. What is this telling you? This is the force
of a wire over a small segment of the wire which has length dl, I is the current through
the wire, and B is the local magnetic field at that location dl, that's what it means. And if you want to know the entire force on
the wire, you have to do the integral along the whole wire. And so you have to do an integral along the
entire wire, and at every portion dl, you have to determine what B is, and you get,
then, a force, which is a vector, and you have to add those vectors vectorially. Could be a pain in the neck, but that's the
basic idea. So now, I want to calculate what the force
was on this wire, roughly, when we ran three hundred amperes through there. And I make a geometry so simple
that we can execute that integral. This was the wire, and we had a current running
through here which was three hundred amperes roughly And we have a magnetic field, which was right
in the gap there, that magnetic field B, and that was two-tenths of a Tesla. Two kilogauss. And that magnetic field was
only operating here. It wasn't operating there. And I make the assumption -- which is a simplifying
assumption -- that that magnetic field was constant over the portion of the wire which
was, say, only ten centimeters. And so I assume here that I have a length
which is 0.1 meters, and that in during -- in this range here, the magnetic
field is constant. I just want to get a rough number for the
force on that wire. So now I can integrate that equation very
easily, because I have assumed that the magnetic field is perpendicular to the direction dl --
because dl is now in this direction -- so the sine of theta is one, so I don't
have to worry about that and so I simply get that the force on this section L, that force, call it F of B if you want to is the current I, which
we have there, we get the length L, which is this length,
multiplied by the magnetic field. There is no sine I anywhere because the angels
are ninety degrees. And so I find that that force is three hundred
times 0.1 times 0.2, so it is thirty times point two, that is about
six Newton. Six Newton is more than
the weight of one pound. And so it is not so surprising that when I
turn this current on, that something, all of a sudden,
pulls that wire down with a weight that is equivalent of a little more than a pound,
almost a pound and a half, actually. And so it's not so surprising
that these supports fell over. So you see that you can turn this quantitatively,
provided that you make some simplifying assumptions about the uniformity of the magnetic field,
and about where the magnetic field is present. Now, I want to
talk about the great 8.02 motor contest. This contest is not part of 8.02x . We are about to start on this great 8.02
motor contest, you got an envelope today, and I'm going to start to tell you,
slowly, about the physics. The goal is, ultimately, to build a motor. If I have a current loop here is a current loop. Current comes in at A, and I'll try to make
it -- make you look at it three-dimensionally, which is not so easy. This is -- current goes out here, at D. This is a current loop. Current go through here, go through here,
go through here, and we turned here. And we have a magnetic field, and we will assume that the magnetic field
is constant throughout in this direction. There is a force right here on this wire,
in the direction I cross B. That force is up. There is a force here, on this wire, which
is, of course, down. Magnetic field is in the same direction, the current is in the opposite direction,
so the force is down. If this wire has a length a, this wire has
a length a, that force, the magnitude of that Force is the current through the wire
times the length of the wire times the B field. We just derived that. There's that integral, we just assume that
the magnetic field is constant everywhere here, there, at ninety-degree angles, so the
sine of theta is one, and so that's the force. What is the force here and
what is the force here? Well, it's zero. Zero here, and it is zero here. Why is that? Because the
cross-product is zero. No matter how you look at it, you can say
dl and B are either in the same direction or in opposite directions. You can also say the drift velocity and B
are either in the same or the opposite direction. It is all the same thing. There is no force here,
and there is no force here. Because that equation that we had that gives
us the magnetic force becomes zero. The sine of that angle is zero. So what's going to happen with this thing?
Well, there is a torque on this system. There is no net force, because this force
up is the same as this force down, but there is a torque which wants to rotate it
in counterclockwise direction. And the magnitude of that torque is, of course,
this force, you remember from 8.01, times the perpendicular distance between
these two forces, and so the magnitude of that torque is I times ab times B
at this moment in time, when the forces are this far apart. Now, this is going to rotate, and so as they
rotate, these forces come closer, and so the torque will become less. Still, it wants to rotate counterclockwise. And there comes a time, ninety degrees later,
that the torque is zero. And I will try to make you see that, again,
in a three-dimensional way, it's not so easy for me. Now, this is D, this has become D, a current
always leaves at D. I'll try to make you see this three-dimensionally. It goes like this a current comes in here, at A, so we get this, and we get this. It doesn't look so bad. And the magnetic field B has not changed,
uniform B in the same direction. So the current now comes in through A, it
has not changed, the only thing is that the loop has rotated ninety degrees. If, now I ask you what the forces are, you
have to go I cross B. I cross B. If you do I cross B here, I cross B, you get
a force which is towards you. Here, you get forces which are in the blackboard. Here you get forces which are up, and here
you get forces which are down. At home, you will have some time to use your
right hand, and do the I cross B, and you will see, then, that, indeed, all these forces
are in the direction that I put them. So now, there is, again, no net force on the
system. There was no net force here, either. But now, there is no torque either. So now, the torque has become zero. If we rotate it a little further, it is possible,
then we start this motor, starts to rotate counter clockwise, comes to this position,
torque goes to zero, but it has enough inertia so it rotates a little further. And now the torque will reverse. And this is something that I leave you alone
with, I don't want to make another drawing and convince you that it reverses. But it's easy to see, because, take this thing,
and just flip it over hundred eighty degrees. The magnetic field hasn't changed, but the
currents in these two sides have changed direction now because whatever is D is here and A is
here. And so the torque reverses, and so it goes
like this, [wssshhht], and then [wsshht] it comes back. And that's not much of a motor. Current meters are very frequently used, they
are in your cars, many more than you think, your, um, your fuel gauge and your temperature,
of the cooling water, are current meters. And a current meter works as follows. We attach to this loop a needle, a handle,
and we calibrate it here. And you can read how many amperes are going
through this meter. It wants to go counterclockwise. Here, we attach a spring and the spring produces
a counter-torque, and so the needle will start to deflect, but come to a halt. But if you double the current, it will go
further. That's the way that a current meter works. And your fuel gauge in your car is a current
meter, except that the level of the fuel is somehow converted into an electric signal, and then it's sent to a current meter,
and that's what you are reading. And it is, of course, calibrated in terms
of how much fuel you have. And your temperature gauge is calibrated in
terms of degrees, whatever, Fahrenheit or whatever. So these current meters are very common, even when we're dealing with something that has
nothing to do with a current. How do you build, now, a motor that works?
How do you get over this torque reversal? Well, it's not only the torque reversal that
is a problem, but there is also the problem that if you could keep this going around,
that these two wires would intertwine, and they would break. You roll it around a hundred times, you can
see what happens at A and D, it will break. So you have to think of a design whereby you
have slipping contacts -- we call them brushes. Suppose I have, here, a conductor which is
connected with A, physically soldered to the wire at A. And here, I have a conductor which is D. So the -- the loop is where you are. Soldered wires coming out the loop is here. But now the battery plus side of the battery is here,
and the minus side of the battery of here, and this is a slipping contact. In practice, we call them brushes. So that immediately takes care of the problem,
that the wires wind up. But there is something else which is very
clever about this design. If the gap between A and D
is an insulator, then, what's going to happen
when this rotates 180 degrees? A, which now is on
the positive side of the battery this is negative, of course, heh? A is now on the
positive side of the battery, if you rotate hundred eighty degrees, A will
be on the negative side of the battery. So now every rotation, the current will, all
by itself, change direction. And we call that a commutator. And so now, what's going to happen is, now
the torque reversal will not occur. If, at the right moment, the current switches
direction, the torque will always want to rotate the loop in exactly the same direction. That's the idea behind a commutator. The great 8.02 motor contest. You have an envelope, when you open it up
-- don't do it now -- you will find in there a copper wire, two meters insulated copper wire, two magnets,
two paper clips, and some wood And the idea is that you try to build a motor
that runs as fast as possible. For every hundred RPM
-- an RPM is a rotation per minute -- for every hundred RPM I'll give you one credit point, with
a maximum of twenty credit points. So if your motor runs two thousand RPM
or more, you get twenty credit points. That is equivalent to two homework assignments. And these credit points come over and above
your course grade. You have my word for that. We'll give you a final course grade, the way
that you've seen in the ground rules, in the first handout, and we add your motor contest,
what you deserved. For every hundred RPM, you get one point,
plus, with a maximum of, uh, of twenty. And we're going to test these motors on the
second of April, and I gave you a handout in which I give you some hints, some ideas. There is one idea that I gave you which you
may ignore, and that is to overcome the torque reversal. you can build a commutator. But that's, uh, that's really not easy. Not only is it not easy, but when you built
a commutator, your system may get a lot of friction, and you may lose more than you gain. There is an alternative solution, which I
mentioned in my handout that you picked up today and that is that you design your motor
in such a way that when the reversal, when the torque reversal occurs, that there is
no current running any more. And when it is half a rotation further, the
torque is there again, the current is there again. So for half the time, you stop the current,
you will see that's very easy, I'll give you some hints how you do that. So you have to weigh that against the possibility
of building a commutator. The bottom line is, the maximum is twenty
credit points. That's an equivalent of two homework assignments. You get it over and above your course grade. And it's also great, fun, believe me. What more do you want? To do physics, get
credit, and have fun. That's what I do every day, that's the great
thing about physics. We have five minutes left, and in those five
minutes, I'm going to demonstrate to you a motor. What you see there is a current loop, I'll
try to make you see it three-dimensionally this is the current loop, and we're going
to run a current in this direction, and we here, have a magnet, north, south, magnetic
field is in this direction. And we, here, have a magnet, north, south,
magnetic field is also in this direction. I'm going to run a current through here, and
if the current is in the blackboard, I cross B -- I is in, cross B, force is up. This side wants to go up. If this side wants to go up, since the magnetic
field is in the same direction here, but the current is hundred eighty degrees in opposite
direction, this force will be down. And so there's a torque on this motor. And you will see that. You will see that go like this. However, when it's hundred eighty degrees
and it swings here, by, it wants to go back, because of the torque reversal. That's the first thing
that I want to show you. And I think I don't need any
changes in the light. So here, we have this loop, and here we have
the two magnets the magnetic field is by no means
uniform by the way it's very strong here,
and it's very strong there. And now I have to power that. Hmm, there we go. I can't -- yeah, I think I know that this one
will come up this side, I'm fairly sure that I have the directions right. Let's first take a look at it. There it goes. So when it's here, notice, it goes up. But now, if I power it here again, wants to
go back. So here, wants to go up, and here, it wants
to go back. So we've got to do something. And that something is a commutator. So if we can somehow reverse the current when
it's here, then it wants to go down again. I'll show you that. So now it's here. And I'll drive the current in the other direction. You ready for that? Did you notice? It now
wants to go down. Now it wants to go down. But when it's here, I have to reverse the
current, it wants to go up. And if I do that with my hand, I can see
whether I can keep this rotating. It may take me a while, but I'll do my best
I can. There it goes. Switch, switch, switch, switch, switch, switch,
switch, switch, switch. Yeah, got it, yeah I got it. I'm a commutator! (class laughs) This motor is going at least
sixty RPM, that's one credit point for me
for this course. Thank you. (applause)
