Yesterday we had two hundred
and twenty-five motors,
and six of those motors went
faster than two thousand RPM,
which is a reasonable
accomplishment.
And the elite is here.
These are the elite,
the six highest.
The winner is,
um, Yungun Lee,
I talked to her on the phone
last night.
If all goes well,
she is here.
Are you here?
Where are you?
There you are.
Why don't you come up so that I
can con- congratulate you in
person.
I thought about the,
the prize for a while,
and I decided to give you
something that is not
particularly high tech,
but come up here,
give me a European kiss,
and another one -- in Europe,
we go three.
OK.
Um, the prize that I have for
you is a thermometer which goes
back to the days of Galileo
Galilei -- come here.
Uh, it was designed in the
early part of the,
um, seventeenth century.
Uh, it doesn't,
uh, require any knowledge of
eight oh two to explain how it
works.
If anything,
you need eight oh one.
It's not a digital thermometer.
But it's accurate to about one
degree centigrade,
and if you come here,
you can tell,
you look at these
floaters, and the highest
floater indicates the
temperature.
It's now seventy-two degrees
here.
And I suggest that you brush up
on your knowledge of eight oh
one so that perhaps next week
you can explain to me how it
works.
[laughter].
And of course tell your
grandchildren about it.
You may want to leave it here.
It's very fragile.
Uh, there is also some package
material here,
so that you can take it home
without breaking it.
So congratulations once more
[applause] and of course
-- [applause].
Terrific.
And you will join us for dinner
on the thirteenth of April with
the other five winners.
Thank you very much.
There are two other people who
are very special who I want to
mention.
And one is a person who is not
enrolled in, uh,
eight oh two,
but he did extremely well,
and he was very generous.
He was not competing.
His name is Daniel Wendel.
His motor went forty-nine
hundred RPM.
And then there was Tim Lo.
Is Tim Lo in the audience?
I hope he's going to be there
at eleven o'clock.
Tim made a motor -- when I
looked at it,
I said to myself,
it'll never run,
but it's so beautiful.
It was so artistic that we
introduced a new prize,
a second prize,
for the most artistic motor,
and Tim Lo definitely is the
one, by far the best,
the most beautiful,
the most terrific artistic
design.
And so for him I bought a book
on modern art -- what else can
it be for someone who built such
a beautiful motor?
It is here for those of you who
want to see it later.
It's very hard to display it on
television because it's so
delicate.
It's like a birdcage that he
built instead of having just --
looks like that it's a birdcage.
It's very nice.
The winning motor I have here,
and I'm going to show you the
winning motor,
and I also want to teach you
some,
some physics by demonstrating
the winning motor to you in a
way that you may never have
thought of.
So this is the winning motor.
And when we start this motor,
the ohmic resistance of the
current loop is extremely low.
So the moment that you connect
it with your power supply,
a very high current will run.
But the moment that the motor
starts to rotate,
you have a continuous magnetic
flux change in these loops,
and so now the system will
fight itself,
and it will immediately kill
the current, which is another
striking example of Faraday's
Law.
I will show you the current of
this motor when I block the
rotor so that it cannot rotate.
It's about one point six
amperes.
And you will see the moment
that I run the motor that that
current plunges by a huge
amount.
Striking example of Faraday's
Law.
So I now have to first show you
this
current, so here you see the
one and a half volts,
and on the right side you see
the current.
There is no current flowing now
because the loop is hanging in
such a way that the,
that it makes no contact with
the battery.
And I'm going to try to make it
-- there it is.
Do you see the one point six
amperes on the right?
The current is so high that due
to the internal resistance of
the power supply,
the voltage also plunges.
But you saw the one point six,
right?
Now I'm going to run the motor.
See, the motor is running now,
and now look at the current.
Current now,
forty milliamperes,
thirty milliamperes,
fifty milliamperes.
It's forty times lower than
when I blocked the rotor.
And so this is one of the
reasons why when you have a,
a motor, whichever motor it is,
it could be just a drill,
you try not to block it all of
a sudden, because an enormous
current will run,
and it can actually
damage the motors.
So you see here how the current
goes down by a factor of forty
between running and not running.
All right.
Electric fields can induce
electric dipoles in materials,
and in case that the,
the molecules or the atoms
themselves are permanent
electric dipoles,
an external electric field will
make an attempt to align them.
We've discussed that in great
detail before when we discussed
dielectrics.
And the degree of success
depends entirely on how strong
the external electric field is
and on the temperature.
If the temperature is low,
you have very little thermal
agitation, then it is easier to
align those dipoles.
We have a similar situation
with magnetic fields.
If I have an external magnetic
field, this can induce in
material
magnetic dipoles.
And it, uh, induces magnetic
dipoles at the atomic scale.
Now in case that the atoms or
the molecules themselves have a
permanent magnetic dipole
moment, then this external field
will make an attempt to align
these dipoles,
and the degree of success
depends on the strength of the
external field,
and again on the temperature.
The lower the temperature,
the easier it is to align them.
So the material modifies the
external field.
This external field,
today I will often call it the
vacuum field.
So when you bring material into
a vacuum field,
the field changes.
The field inside is different
from the external field,
from the vacuum field.
I first want to remind you of
our definition of a magnetic
dipole moment.
It's actually very simple how
it is defined.
If I have a current --
a loop could be a rectangle,
it doesn't have to be a circle
-- and if the current is running
in this direction,
seen from below clockwise,
and if this area is A,
then the magnetic dipole moment
is simply the current times the
area A.
But we define A according to
the, the vector A,
according to the right-hand
corkscrew rule.
If I come from below clockwise,
then the vector A is
perpendicular to the surface and
is then pointing upwards.
And so the magnetic dipole
moment,
for which we normally write mu,
is then also pointing upwards.
And so this is a vector A,
which is this normal according
to the right-hand corkscrew.
And if I have N of these loops,
then the magnetic dipole moment
will be N times larger.
Then they will support each
other if they're all in the same
direction.
I first want to discuss with
you diamagnetism.
Diamagnetism.
All materials,
when you expose them to an
external magnetic field,
will to some degree oppose that
external field.
And they will generate,
on an atomic scale,
an EMF which is opposing the
external field.
Now you will say,
yes, of course,
Lenz's Law.
Wrong.
It has nothing to do with
Lenz's Law.
It has nothing to do with the
free electrons in conductors
which produce an eddy current
when there is a changing
magnetic field.
I'm not talking about a
changing magnetic field,
I'm talking about a permanent
magnetic field.
So when I apply a permanent
magnetic field,
in all materials,
a magnetic dipole moment is
induced to oppose that field.
And there is no way that we can
understand that with eight oh
two.
It can only be understood with
quantum mechanics.
So we'll make no attempts to do
that, but we will accept it.
And so the magnetic field
inside the material is always a
little bit smaller than,
than the external field,
because the dipoles will oppose
the external field.
Now I will talk about
paramagnetism.
Paramagnetism.
There are many substances
whereby the atoms and the
molecules themselves have a
magnetic dipole moment.
So the atoms themselves or the
molecules, you can think of them
as being little magnets.
If you have no external field,
no vacuum field,
then these dipoles
are completely chaotically
oriented, and so the net el-
magnetic field is zero.
So they are not permanent
magnets.
But the moment that you expose
them to an external magnetic
field, this magnetic field will
try to align them.
And the degree of success
depends on the strength of that
field and on the temperature.
The lower the temperature,
the easier it is.
And so if you had a magnetic
field, say, like so -- this is
your B field,
this is your vacuum field --
and you bring in there
paramagnetic material,
then there is the tendency
for the north pole to go a
little bit in this direction.
And so these atomic magnets,
then, would on average try to
get the north pole a little bit
in this direction.
Or, if I speak the language of
magnetic dipole moments,
then the magnetic dipole would
try to go a little bit in this
direction.
If you remove the external
field of a paramagnetic
material, immediately there is
complete, total chaos,
so there is no permanent
magnetism left.
If you bring paramagnetic
material in a non-uniform
magnetic field,
it will be pulled towards the
strong side of the field.
And this is very easy to,
to see how that works.
Suppose I have a magnet here,
and let this be the north pole
of the magnet and this the south
pole.
And so the magnetic field is
sort of like so.
Notice right here it's
very non-uniform.
And I bring some paramagnetic
material in there.
Let's say -- think of it as
just one atom there.
It's not to scale,
what I'm going to draw.
And here is that one atom,
and this one atom now is
paramagnetic,
has its own magnetic dipole
moment.
And this magnetic dipole
moment, now, would like to align
in this direction to support the
field.
The field is trying to push it
in that direction.
Let's suppose it is in this
direction.
So if we look from above,
the current then in this atom
or in this molecule is running
in this direction.
Seen from above,
clockwise.
So that would be ideal
alignment of this atom or this
molecule in that external field.
This current loop will be
attracted -- it wants to go
towards the magnet.
Let's look at this point here.
That point, the current is
going in the blackboard.
So here is that current I.
And the magnetic field is like
so, the external magnetic field
is like so.
So in what direction is the
Lorentz force?
It's always in the direction I
cross B.
And I cross B,
I cross B is in this direction.
That's the direction of the
Lorentz force.
So right here,
there is a force on the loop in
this direction.
So therefore right here,
there is a force on the loop in
this direction,
on the current loop.
And so everywhere around this
loop, there is a force that is
pointing like this,
and so there clearly is a net
force up.
And so this matter wants to go
towards the magnet.
Another way of looking at this
is that this current loop is all
by itself a little magnet,
whereby the south pole is here
and the north pole is there,
because this is the direction
of the magnetic dipole moment.
And the north pole attracts the
south pole.
That's another way of looking
at it.
That's the reason why magnets
attract each other,
why north and south pole
attract each other,
and why north and north poles
repel each other.
That's exactly the reason.
It is the current that is
flowing, it is the Lorentz force
that causes the attraction or
the repelling force.
So paramagnetic material is
attracted by a magnet.
Essential is that this field is
non-uniform.
And diamagnetic material,
of course, will be repelled,
will be pushed away from the
strong field,
because in paramagnetic -- in
diamagnetic material,
this current will be running in
the opposite direction,
because it opposes the external
field whereas paramagnetism
supports it.
We have a third form,
and the third form of magnetism
-- it's actually the most
interesting -- is
ferromagnetism.
In the case of ferromagnetism,
we again have that the atoms
have themselves permanent dipole
moments.
But now, for very mysterious
reasons which can only be
understood with quantum
mechanics, there are domains
which have the
dimensions of about a tenth of
a millimeter,
maybe three tenths of a
millimeter, whereby the dipoles
are hundred percent aligned.
And these dipoles,
domains, which are in one
direction, are uniformly
distributed throughout the
ferromagnetic material,
and so there may not be any net
magnetic field.
If I have here -- if I try to
make a sketch of those domains,
something like this,
then perhaps here all these
dipoles would all be hundred
percent aligned in this
direction, but for instance
here, they will all be aligned
in this direction.
And the number of atoms
involved in such a domain is
typically ten to the seventeen,
maybe up to ten to the
twenty-one atoms.
So if now I apply an external
field, these domains will be
forced to go in the direction of
the magnetic field,
and of course the degree of
success depends on the strength
of
the external field,
the strength of the vacuum
field, and on the temperature.
The lower the temperature,
the better it is,
because then there is less
thermal agitation,
which of course adds a certain
rando- randomness to the whole
process.
So when I apply an external
field, these domains as a whole
can flip.
Inside the ferromagnetic
material, the magnetic field can
be thousands of times stronger
than it
is in the vacuum field.
And we will see some examples
of that today.
If you remove the external
field, in the case of
paramagnetism,
you have again complete chaos
of the dipoles.
That's not necessarily the case
with ferromagnetism.
Some of those domains may stay
aligned in the direction that
the external field was forcing
them.
If you very carefully remove
that external field,
undoubtedly some domains will
flip back, because of the
temperature, there is always
thermal agitation.
Some may remain oriented,
and therefore the material,
once it has been exposed to an
external magnetic field,
may have become permanently
magnetic.
And the only way you can remove
that permanent magnetism could
be to bang on it with a hammer,
and then of course these
domains will then get very
nervous, and then they will
randomize themselves.
Or you can heat them up,
and then you can also undo the
orientation of the domains.
The domains themselves will
remain, but then they average
out not to produce any permanent
magnetic field.
So for the same reason that
paramagnetism is pulled towards
the strong field,
in case that we have a
non-uniform magnetic field,
ferromagnetism of course will
also be pulled towards the
strong field,
except in the case of
ferromagnetism,
the forces with which
ferromagnetic material is pulled
towards the magnet,
way larger than in case of
paramagnetic material.
If I take a paperclip -- you
can do that at home,
you can hang a paperclip on the
south pole of your magnet or the
north pole of your magnet --
you all have gotten magnets in
your motor kit,
so you can try that at home.
Take a paperclip,
hang it on the magnets.
Doesn't matter on which side
you hang it, because
ferromagnetic material is always
pulled towards the strong field.
If you hang a few of those
paperclips on there and you very
carefully and slowly remove them
-- don't hit them with a hammer
yet -- you may actually notice
that after you remove them that
the paperclips themselves have
become magnetic.
You can actually try to hang
them on
each other, make a little
chain.
But drop them on the floor a
few times and that magendas-
magnetism will go away.
So what you have witnessed then
is that some of those domains
remained aligned due to your
external field.
With paramagnetism,
there is no way that you can
hang paramagnetic material under
most circumstances on a magnet.
There is one exception.
I will show you the exception
later today.
And the reason is that the
forces involved with
paramagnetic material
in general are only a few
percent of the weight of the
material itself.
So if you take a piece of
aluminum and you have a magnet,
aluminum will not stick to a
magnet.
There is a force.
Aluminum will be attracted by
the magnet, but the force is way
smaller than the weight of the
aluminum, so it won't be able to
pick it up, unlike ferromagnetic
material, which you can pick up
with a magnet.
So what I could demonstrate to
you, for one thing,
I could take a bar magnet and
show you that paperclips are
hanging on this.
I could also show you that
aluminum is not hanging on this.
But you won't find that very
exciting.
And therefore I decided on a
different demonstration,
whereby my goal is to show you
that ferromagnetic material is
pulled with huge forces towards
the strong magnetic field,
provided that I have a magnetic
field which is non-uniform.
And the way I will do that is
with this piece of ferromagnetic
material.
And this piece of ferromagnetic
material is actually quite
heavy.
And you are going to tell the
class how heavy it is.
Be very careful.
What do you think?
Wow!
Good for you!
[laughter].
Do it again!
Sounds go-- looks great.
[laughter].
It's fifteen kilograms.
Fifteen kilograms of
ferromagnetic material.
It is not a permanent magnet.
There may be a little bit of
permanent magnetism left,
of course, because once you
have exposed it to an external
field, yes, there may be some
permanent magnetism left.
So now I'm going to hold this
-- let's first make sure that
nothing happens to Galileo's
thermometer.
So we're going to put this
here.
See what the temperature is --
oh man, it's going up.
I must be sweating here.
Seventy-four degrees,
yeah, seventy-four degrees now.
OK, so here is my magnet,
producing about three hundred
twenty gauss.
But what counts is that the
magnetic field is non-uniform
here and also here.
And so I am going to turn on
the
magnet -- I believe I have to
push a button here.
And the first thing I will do
is now power this magnet.
So this is a solenoid.
I put my hand in here,
my hand is paramagnetic,
it's not being sucked in.
Really it isn't.
I feel nothing.
The force is -- I can't even
feel anything.
But I'm not ferromagnetic,
thank goodness.
Now this one.
*Whssht*, fifteen kilograms,
just sucked in like that.
And I'm very lucky that when
it's overshoots here that it
wants to go back,
because it always wants to go
to the strongest field.
Doesn't matter whether you have
it here or there.
The reason why that's lucky,
because if that were not the
case, this fifteen kilogram bar
would go like a bullet coming
out of here.
So the one thing you don't want
to do when it goes in there,
you don't want to break the
current, because then it would
come out as a bullet.
And I'm not going to do that,
believe me.
But I want to show you that --
there it goes.
It's amazing,
ferromagnetic
material.
*Aagh*.
OK.
So ferromagnetic material,
there's enormous force.
If you have a s- a field that
is -- has a strong gradient,
that it's very non-uniform,
is sucked, pulled towards the
strong side.
That's why it hangs on magnets.
That's the basic idea.
I have another demonstration.
And another demonstration is to
make you sort of see in a
non-kosher way
magnetic domains.
But I will tell you why it's
non-kosher.
I have here an array of eight
by eight magnetic needles,
compass needles.
And you're going to see them
there.
And I will change the situation
so that you have better light.
And when I have an external
magnetic field and I march over
here a little,
and I just let it go,
and wait, you will see areas
whereby these magnetic needles
point in the same direction and
you will see areas where they
point in a different direction.
We'll just give it some chance.
And so that may make you think
that this is the way that
domains are formed in
ferromagnetic material.
Oh, in fact we have now a
situation that almost all are
aligned in this direction,
and there's only a group here
that is pointing in this
direction.
I can change that,
of course, by changing the
magnetic field.
Why is this not really a kosher
demonstration to convince you
that domains exist?
First of all,
there is no thermal agitation,
whereas in ferromagnetic
material there is thermal
agitation.
Some may be oriented like this
and others like that,
where here you only have two
preferred directions.
You don't need quantum
mechanics for that,
simply a matter of minimum
energy considerations.
And so they either are pointed
like
this or they are pointed like
that, and so already that shows
you that it's very different
from ferromagnetism.
But the reason why we show it
to you is it still gives you an
interesting idea of the fact
that you can have various
orientations and that they come
in groups.
That the groups stick together
and are not all in the same
direction.
But as I said,
it is not really a good way to
explain to you why there are
domains in ferromagnetic
material.
Ah, now you see again,
you have some nicely aligned
here and others are in very
different direction here.
So the basic idea is there.
It's a nice demonstration,
but it shows you something that
really is not related to
ferromagnetism.
The demonstration that is one
of my favorites,
one of my absolute favorites,
is one whereby I can make you
listen
to the flip-over of these
domains.
I have ferromagnetic material
inside a coil.
I have here a coil and I'm
going to put ferromagnetic
material in here.
And I have here a loudspeaker
-- an amplifier as well,
called it an amplifier.
And this is a loudspeaker.
Let's first assume there is no
ferromagnetic material in
there.
That's the way I will start the
demonstration.
And I approach this with a
magnet, and I go very fast.
*Whssht*, what will happen?
Faraday will say,
oh, there's a magnetic flux
change, and there will be an EMF
in this coil.
That means there will be a
current in this coil,
induced current.
And it will be amplified and
you will hear some sissing
noise.
And you will hear that.
If, however,
I come in very slowly,
you won't hear anything,
because D phi DT is then so
low, because the time scale of
my motion is so large,
that you won't hear any
current.
The induced current is
insignificantly small.
Because remember the induced
current is proportional to the
induced EMF, and the induced EMF
is proportional to the time
change of the magnetic flux.
So I can make that flux change
very, very small if I bring it
in very slowly.
Now I will put in the
ferromagnetic material,
and I will approach it
again very slowly.
And now, there comes a time
that some of those domains go
*cluk*, *cluk*.
But when the domains flip over,
there is a magnetic flux change
inside the material,
and so the magnetic flux change
means D phi DT,
and it's on an extremely short
time scale.
And so now you get an EMF,
you get a current going through
the wire, and you hear a
cracking noise over the
loudspeaker.
And for every group of domains
that flip, you can hear that.
And that's an amazing thing
when you think about it,
that some ten to the twenty
atoms go
clunk and that you can hear
that.
And so this is what we're going
to do here, and I will do it
then in, in several steps,
so that you first can hear the
noise if I don't have
ferromagnetic material,
and then -- so here is the,
here's the coil.
This is a very small coil.
And here is a magnet.
And I'll come very fast towards
the coil.
What you heard now is Faraday's
Law.
You simply have a magnetic flux
change in the coil -- oh,
I shouldn't touch it.
Now I come in very slowly,
and go away very slowly.
You hear nothing.
D phi DT is just too low.
Now I put in the ferromagnetic
material.
Put it inside the coil.
And now I approach it again,
very slowly.
There they go.
You hear them?
Those are, those are domains
that go.
I'll come in with the other
side.
There it goes,
the domains.
Isn't that amazing?
You hear atoms switch,
groups of atoms.
I'll turn it over again.
Now they flip back.
They don't like it that that's
there.
This is called the Barkhausen
effect.
I find it truly amazing that
you hear groups of atoms,
ten to the twenty atoms at the
time, they flip over,
and when they do,
there is a magnetic flux change
inside the ferromagnetic
material, is sensed by the coil,
and you hear a current.
And if I do it fast,
uh, these, these,
these, these domains go
haywire.
They go nuts now.
Imagine that you were a domain
and I would treat you that way.
You'd go *cluk*,
*cluk*, *cluk*,
*cluk*, *cluk*.
But the fact that you can hear
it is absolutely amazing,
isn't it.
So that's actually a nice way
of demonstrating that these
domains exist.
If you did that with
faramagnetic- paramagnetic
material, you wouldn't hear
that.
So in all cases,
whether we have diamagnetic
material or paramagnetic
material or ferromagnetic
material, uh,
the magnetic field inside is
different from what the field
would
be without the material.
And what the field would be
without the material we've
called external field.
I've called it vacuum field.
And in many cases,
but not all -- next lecture I
will discuss the issues of not
all -- in many cases but not all
cases, is the field inside the
material proportional to the
vacuum field.
And if that is the case,
then you can write down that
the field inside is linearly
proportional -- so this is the
field inside the material,
regardless of whether it's
diamagnetic or paramagnetic or
ferromagnetic,
is proportional to the vacuum
field.
I will write down vacuum for
this.
And this proportionality
constant I call kappa of M.
I -- our book calls it K of M.
And it's called the relative
permeability.
And so now we can look at these
values for the relative
permeability and we can
immediately understand now the
difference between
diamagnetic material,
paramagnetic material,
and ferromagnetic material.
Since in the case of
diamagnetic material and
paramagnetic material,
the B field inside is only
slightly different from the
vacuum field,
it is common to express kappa
of M in terms of one plus
something which we call the
magnetic susceptibility,
which is xi of M.
Because if it is very close to
one, then it is easier to simply
list xi of M.
And let's look at diamagnetic
material.
Notice that these values for xi
of M are all negative -- of
course, they have to be
negative, otherwise it wouldn't
be diamagnetic.
It means that the field inside
is slightly, a hair smaller than
the vacuum field,
because these induced dipoles
oppose the external field,
remember.
It has nothing to do with
Lenz's Law,
but they oppose it
nevertheless.
And so you express it in terms
of the, um, magnetic
susceptibility,
and so you have to take one
minus one point seven times ten
to the minus four to get kappa
of M, which is very close to
one.
If now you go to paramagnetic
materials, the minus signs
become plus.
Again, the numbers are small.
But the fact that it is plus
means that inside paramagnetic
material, the magnetic field is
a little, a
hair larger than the vacuum
field.
But now if you go to
ferromagnetic material,
it is really absurd to ever
list the value for xi of M,
because xi of M is so large
that you can forget about the
one, and so xi of M is about the
same as kappa of M.
And so you deal there with
numbers that are a hundred,
a thousand, ten thousand,
and even larger than ten
thousand.
That means that if kappa of M
is ten thousand,
you would have a field inside
ferromagnetic material that is
ten thousand times larger than
your vacuum field.
Next lecture I will tell you
that there is a limit to as far
as you can go,
but for now we will,
we will leave it with this.
So paramagnetic and
ferromagnetic properties depend
on the temperature.
Diamagnetic properties do not
depend on the temperature.
So at very low temperatures,
there is very little thermal
agitation, and so you can then
easier align
these dipoles,
and so the values for kappa of
M will then be different.
For ferromagnetic material,
if you cool it,
you expect the kappa of M going
up, so you got a stronger field
inside.
So it's temperature-dependent.
If you make the material very
hot, then it can lose completely
its ferromagnetic properties.
What happens at a certain
temperature, that these dosmain-
domains fall
apart, so the domains
themselves no longer exist.
They annihilate.
And that happens at a very
precise temperature.
It's very strange.
That's also something that is
very difficult to understand,
and you need quantum mechanics
for that too.
But at a certain temperature,
which we call the Curie
temperature, which for iron is a
thousand forty-three degrees
Kelvin, which is seven hundred
seventy degrees centigrade,
all of a sudden the domains
disappear and the material
becomes paramagnetic.
In other words,
if ferromagnetic material would
be hanging on a magnet and you
would heat it up above the Curie
point, it would fall off.
It would become paramagnetic,
but paramagnetic material in
general doesn't hang on a
magnet, because the forces
involved are quite small.
And the change is very abrupt,
and I am going to show that to
you with a demonstration.
I have a ferromagnetic nut.
It's right there.
You will see it very shortly.
And this nut,
or washer, hanging on a steel
cable, and there is here a
magnet.
I don't know whether this is
north or south.
It doesn't matter.
And here we have a thermal
shield.
And so this washer is against
the thermal shield,
because it's being attracted.
It wants to go towards the
strong magnetic field.
It's ferromagnetic.
So it will be sitting here.
And now I'm going to heat this
up above the Curie point,
seven hundred seventy degrees
centigrade, and you will
see it fall off.
And when it cools again,
it goes back on again.
So I can make you see
ferromagnetic properties
disappear.
And let me make sure I have the
proper settings.
I see nothing.
I see nothing.
But there it is.
So here is this nut,
and here is this shield,
and the magnet is behind it,
you can't see it,
but it's right there.
And so it goes against it,
right, it goes just towards the
magnetic poles.
It goes into the strong
magnetic field.
The magnetic field is
non-uniform outside a magnet,
and it goes towards it.
And so now I'm going to heat
it.
It will take a while,
because, um,
seven hundred seventy degrees
centigrade is not
so easy to achieve.
The three most common
ferromagnetic materials are
cobalt, nickel,
and iron.
Nickel has a Curie point of
only three hundred fifty-eight
degrees centigrade,
so if this were nickel -- ooh.
If this were nickel -- uh-uh.
[laughter].
Oh, you like that,
huh.
I think I need strong hands.
A strong hand is coming.
OK.
I think I fixed it.
I'm a big boy,
I did it myself today.
I lost my pen,
but that's a detail.
OK, let's try again.
So I'm going to heat it up,
and I was mentioning that,
um, nickel has a Curie point of
three hundred fifty-eight
degrees centigrade.
So that's quite low.
This is seven hundred seventy.
Cobalt is fourteen hundred
degrees Kelvin Curie point.
Gadolinium is a very special
material.
Gadolinium is ferromagnetic in
the winter, when the temperature
is below sixteen degrees
centigrade, but it is
paramagnetic in the summer,
when the temperature is above
sixteen degrees centigrade.
It's beginning to be red-hot
now.
Seven hundred seventy degrees
centigrade, you expect some
visible light in the form of red
light -- there it goes.
And I will keep it heating,
I will keep the torch on it,
so that you can see that indeed
it's no longer attracted by the
magnet.
And the moment that I stop
heating it, it will very quickly
cool.
It will become ferromagnetic
again, and it will go back.
Just watch it.
There it goes.
So now it's again
ferromagnetic.
So the transition is extremely
sharp.
All right.
Uh, OK.
So paramagnetic materials,
as I mentioned several times,
in general cannot hang on a
magnet.
The attractive force is
there's not enough.
To hang on a magnet,
the force has to be larger than
its own weight.
And diamagn- diamagnetic
materials is of course
completely out because
diamagnetic materials are always
pushed towards the weak part of
the field.
It's only paramagnetic
materials and ferromagnetic
materials that experience a
force towards the strong part of
the field if the field itself is
non-uniform.
Now there is one very
interesting exception.
And I want to draw your
attention to this,
um, transparency here.
Look here at oxygen at one
atmosphere.
Oxygen at one atmosphere and
three hundred degrees Kelvin has
a value for xi of M which is two
times ten to the minus six.
But now look at liquid oxygen
at ninety degrees Kelvin.
That value is eighteen hundred
times larger than this value.
Why is that so much higher?
Well, liquid,
in general, is about thousand
times denser than gas at one
atmosphere.
So you have thousand times more
dipoles per cubic meter that in
principle can align.
And so clearly you expect an
immediate one-to-one
correspondence between the
density, how many dipoles you
have per cubic meter,
and the value for kappa M --
for xi of M.
And so you see indeed that this
value is substantially larger.
The reason why it is more than
a factor of thousand higher is
that the temperature is also
lower.
You go from three hundred
degrees to ninety degrees,
and that gives you another
factor of two,
because when the temperature is
lower, there is less thermal
agitation, and so the external
field can align the dipoles more
easily.
And so that's why you end up
with a factor of eighteen
hundred.
Even though this value for xi
of M is extraordinarily high for
a
paramagnetic material,
notice that the field inside
would only be point three five
percent higher than the vacuum
field, because if xi of M is
three point five times ten to
the minus three,
that means that the field
inside is only point three five
percent higher than the vacuum
field.
But that is enough for liquid
oxygen to be attracted by a very
strong magnet,
provided that it also has a
very non-uniform field outside
the magnet.
And so the force with which
liquid oxygen is pulled towards
a magnet can be made larger than
the weight of the liquid oxygen.
And so I can make you see today
that I can have liquid oxygen
hanging from a magnet.
And that's what we are going to
do here.
Make sure I have the right
setting.
Ah, this is it.
Now we're going to have some
changes in the lights.
So there you see the two
magnetic poles.
It's a electromagnet.
And so we can turn the magnetic
field on at will.
So here are the poles of the
magnet.
And the first thing I will do
is very boring.
I will throw some,
uh, liquid nitrogen between the
poles.
Now I don't have the value for
liquid nitrogen there,
but nitrogen is diamagnetic,
so it's not even an issue.
Diamagnetic material is pushed
away from the strong field.
So even though the value for xi
of M will be very different for
liquid nitrogen than it is for
gaseous nitrogen,
it doesn't matter.
So certainly it will be pushed
out.
So that's the first thing I
want to do, just to bore you a
little bit.
Because I have to keep you on
the edge of your seat before
you're going to see this oxygen,
which will be hanging in there.
So let's first power this
magnet -- I hope I did that --
yes, I think I did.
And here comes the liquid
nitrogen.
Boring like hell,
just falls through.
Now comes the oxygen.
Liquid oxygen.
It's hanging in there.
I challenge you,
you've never in your life seen
liquid hanging on a magnet.
You can tell your parents about
it -- and of course your
grandchildren.
It's hanging there.
I'll put some more in -- make
sure I have the right stuff,
yeah.
Put some more in.
There is liquid oxygen.
When I break the current,
it's no longer a magnet,
it will fall of course.
Don't worry,
you'll get more.
Who has ever in his life seen a
liquid hang on a magnet?
It's paramagnetic,
it's not ferromagnetic,
but because the density is so
high and because it's so cold,
the value for xi of M is high
enough that the force on it is
larger than its own weight.
If you do this with aluminum,
not a chance in the world.
Aluminum will not hang in
there, even though aluminum,
as you can see there,
is paramagnetic.
But the value two times ten to
the minus five is way too small,
and it will not stick to a
magnet.
OK.
You have something to think
about.
I will see you Friday.
