Consider a rod of mass m, and suppose
I apply a force to this rod.
Let's say a force like that.
So we know that as a result of that applied force, the center
of mass of the rod, which we can imagine is right at the center
the rod, will translate with some acceleration, such
that the vector f is equal to the mass
of the rod times the acceleration
of the center of mass.
Now recall that for a rigid body,
this equation will be true regardless of where on the rod
I apply the force.
So for example, if I draw the rod again over here,
and I apply the same force, vector f, but I apply it,
let's say, on the right hand side,
I'll still have the same f equals ma.
All I specify with f is its magnitude and direction.
But for a rigid body, no matter where on the body
I apply that force, the acceleration
of the center of mass will be the same.
Now, we know from experience, however,
that the motion of the rod is different
if I push it at the center at one end or at the other end.
The point is, though, that the motion, the overall motion,
the overall translation of the object
doesn't just involve the translation
of the center of mass, but it also involves some rotation,
in general.
So in fact, there is a theorem called Chasles' theorem, which
tells us that the most general displacement of a rigid body
can be split into the translation
of the center of mass and a rotation about the center
of mass.
Our f equals ma relation tells us
how an applied force affects the first part of the translation
of the center of mass.
But how does that applied force affect
the rotation of the rigid body?
We'll see that this depends not only on the magnitude
and direction of the force, but also on where
the force is applied, OK?
That's different than the translation
of the center of mass, which only
depends upon what the force is.
The rotation about the center of mass
depends both upon the force itself and where on the object
that it's applied.
In fact, in the next few lessons,
we'll see that there's a special equation of motion
for describing rotational motion.
It's analogous to Newton's Second Law of Motion,
analogous to f equals ma, applying to rotational motion.
And we write that relationship.
Its rotational equation of motion
is written as tau, which is a vector,
is equal to i times alpha, which is a vector.
So tau is a new quantity we haven't talked
about before called the torque.
It's a vector.
i is the moment of inertia that we've already encountered,
and alpha is the angular acceleration
of the rotational motion.
Now, tau is a sort of rotational analog to the force,
and it depends on not just the force itself,
but on where the force is applied.
Computing the torque, tau, depends upon something
called a vector product or a cross product.
It's a way of multiplying two vectors together
to produce a third vector.
In that way, it's different than the dot product or scalar
product that we discussed earlier,
where we multiply two vectors together and get
a scalar or a pure number.
This is a different operation, the vector product
or cross-product.
Torque is the first physical quantity we've encountered,
but it won't be the last, that involves a cross-product
in its definition.
And so, before giving you a formal definition of torque,
we'll first review the mathematics of cross-products,
and we'll do that in the next lesson.
Now, the angular acceleration, alpha,
tells us about how the rotational motion changes.
Again, just like in f equals ma, where
we could divide the two sides of this equation
into dynamics and kinematics.
Kinematics is telling us about a geometrical description
of the motion, or the translation of motion,
and the dynamics f is telling us about how
the applied forces cause changes in the motion, changes
in the kinematics.
Likewise, for rotational motion, the angular acceleration,
alpha, tells us about the geometry
of the rotational motion, and specifically
how the rotational motion is changing,
and the torque is telling us about the application of forces
and how that causes changes in the rotation of motion.
So that leaves one other quantity,
which is the moment of inertia.
And I want to talk about what that means for just a moment.
So the term "inertia," the term "inertia" in physics
represents a resistance to an applied force.
It tells us how difficult it is to change an object's motion.
So for example, suppose I have two blocks, one of mass m
and another that's 10 times as massive.
So 10m.
Newton's Second Law, f equals ma,
tells us that if I want to accelerate the heavier
mass to the same rate that I do with a smaller mass,
I'll need to apply a force that's 10 times larger.
So for translation of motion, the mass m
represents the notion of inertia, the resistance
to a force.
It tells us how much force we have
to apply to achieve a certain change in motion.
Now, for rotational motion, that role
is played by the moment of inertia i.
That tells us how difficult it is to change
the rotation of an object.
If I increase the moment of inertia by a factor of 10,
then I'll need a torque that is 10 times larger in order
to achieve the same change in rotational motion,
the same angular acceleration.
But recall that our definition of moment of inertia
for some rigid body is, if I break up
the rigid body into a bunch of little pieces,
and for each piece I take the product
of the mass of that piece, delta mj, times the perpendicular
distance of that piece from the rotation
axis-- I call that rj-- and if I sum
that over the entire object, the entire body, that
gives me my moment of inertia.
Well, so-- sorry, this is r squared.
So it's the mass of each element times the distance
of the axis squared, delta mj times rj squared.
Now, I can increase the moment of inertia by a factor of 10
by increasing the total mass of the object,
but you can see from this equation
that I can also do it with the same mass
by changing the location of the mass.
If I increase the r's, if I move the mass, the same mass,
but I move it to be farther away from the rotation axis,
that also achieves an increase in the moment of inertia.
So what that tells is that for rotational motion,
it's not just the amount of mass that matters,
but also how that mass is distributed.
OK, so in that sense, rotational inertia
is different than translational inertia.
For translational motion, all that matters is the mass.
If I increase the mass by a factor of 10,
then it will become a factor of 10
more difficult to get that object to accelerate.
I need a factor of 10 larger force.
But with rotational motion, I can
increase the notion of inertia.
I can make it more difficult to change the rotation of motion
either by changing the mass, by increasing it,
or by making the distribution of mass
be further away from the rotation axis.
So as an example, imagine if you were rolling a wheel up a hill.
It's different if I have a wheel whose mass is distributed
evenly over the whole disk, or if I have
all of the mass in the rim.
If all of the mass is in the rim, then from this equation,
we see the moment of inertia is larger for the same amount
of total mass.
And so it's much more difficult to roll a wheel up the hill
if all of the mass is in the rim than it
is if the mass is distributed evenly over the wheel.
So our rotational equivalent to Newton's Second Law
is, tau equals i alpha, the torque
equals the moment of inertia times the angular acceleration.
In the next few lessons, we'll see how torque is defined,
and we'll derive this expression for the dynamics of rotation
of motion and see how to apply it.