Let's see if we can use what we know about springs now to
get a little intuition about how the
spring moves over time.
And hopefully we'll learn a little bit
about harmonic motion.
We'll actually even step into the world of differential
equations a little bit.
And don't get daunted when we get there.
Or just close your eyes when it happens.
Anyway, so I've drawn a spring, like I've done in the
last couple of videos.
And 0, this point in the x-axis, that's where the
spring's natural resting state is.
And in this example I have a mass, mass m,
attached to the spring.
And I've stretched the string.
I've essentially pulled it.
So the mass is now sitting at point A.
So what's going to happen to this?
Well, as we know, the force, the restorative force of the
spring, is equal to minus some
constant, times the x position.
The x position starting at A.
So initially the spring is going to pull
back this way, right?
The spring is going to pull back this way.
It's going to get faster and faster and faster and faster.
And we learned that at this point, it has a lot of
potential energy.
At this point, when it kind of gets back to its resting
state, it'll have a lot of velocity and a lot of kinetic
energy, but very little potential energy.
But then its momentum is going to keep it going, and it's
going to compress the spring all the way, until all of that
kinetic energy is turned back into potential energy.
Then the process will start over again.
So let's see if we can just get an intuition for what x
will look like as a function of time.
So our goal is to figure out x of t, x as a function of time.
That's going to be our goal on this video and
probably the next few.
So let's just get an intuition for what's happening here.
So let me try to graph x as a function of time.
So time is the independent variable.
And I'll start at time is equal to 0.
So this is the time axis.
Let me draw the x-axis.
This might be a little unusual for you, for me to draw the
x-axis in the vertical, but that's because x is the
dependent variable in this situation.
So that's the x-axis, very unusually.
Or we could say x of t, just so you know x is a function of
time, x of t.
And this state, that I've drawn here, this is at time
equals 0, right?
So this is at 0.
Let me switch colors.
So at time equals 0, what is the x position of the mass?
Well the x position is A, right?
So if I draw this, this is A.
Actually, let me draw a line there.
That might come in useful.
This is A.
And then this is going to be-- let me try to make it
relatively-- that is negative A.
That's minus A.
So at time t equals 0, where is it?
Well it's at A.
So this is where the graph is, right?
Actually, let's do something interesting.
Let's define the period.
So the period I'll do with a capital T.
Let's say the period is how long it takes for this mass to
go from this position.
It's going to accelerate, accelerate, accelerate,
accelerate.
Be going really fast at this point, all kinetic energy.
And then start slowing down, slowing down, slowing down,
slowing down.
And then do that whole process all the way back.
Let's say T is the amount of time it takes to do that whole
process, right?
So at time 0 today, and then we also know that at time T--
this is time T-- it'll also be at A, right?
I'm just trying to graph some points that I know of this
function and just see if I can get some intuition of what
this function might be analytically.
So if it takes T seconds to go there and back, it takes T
over 2 seconds to get here, right?
The same amount of time it takes to get here was also the
same amount of time it takes to get back.
So at T over 2 what's going to be the x position?
Well at T over 2, the block is going to be here.
It will have compressed all the way over here.
So at T over 2, it'll have been here.
And then at the points in between, it will be at x
equals 0, right?
It'll be there and there.
Hopefully that makes sense.
So now we know these points.
But let's think about what the actual function looks like.
Will it just be a straight line down, then a straight
line up, and then the straight line down, and then a
straight line up.
That would imply-- think about it-- if you have a straight
line down that whole time, that means that you would have
a constant rate of change of your x value.
Or another way of thinking about that is that you would
have a constant velocity, right?
Well do we have a constant velocity this entire time?
Well, no.
We know that at this point right here you have a very
high velocity, right?
You have a very high velocity.
We know at this point you have a very low velocity.
So you're accelerating this entire time.
And you actually, the more you think about it, you're
actually accelerating at a decreasing rate.
But you're accelerating the entire time.
And then you're accelerating and then you're decelerating
this entire time.
So your actual rate of change of x is not constant, so you
wouldn't have a zigzag pattern, right?
And it'll keep going here and then you'll have a point here.
So what's happening?
When you start off, you're going very slow.
Your change of x is very slow.
And then you start accelerating.
And then, once you get to this point, right here, you start
decelerating.
Until at this point, your velocity is exactly 0.
So your rate of change, or your slope, is going to be 0.
And then you're going to start accelerating back.
Your velocity is going to get faster, faster, faster.
It's going to be really fast at this point.
And then you'll start decelerating at that point.
So at this point, what does this point correspond to?
You're back at A.
So at this point your velocity is now 0 again.
So the rate of change of x is 0.
And now you're going to start accelerating.
Your slope increases, increases, increases.
This is the point of highest kinetic energy right here.
Then your velocity starts slowing down.
And notice here, your slope at these points is 0.
So that means you have no kinetic
energy at those points.
And it just keeps on going.
On and on and on and on and on.
So what does this look like?
Well, I haven't proven it to you, but out of all the
functions that I have in my repertoire, this looks an
awful lot like a trigonometric function.
And if I had to pick one, I would pick cosine.
Well why?
Because when cosine is 0-- I'll write it down here--
cosine of 0 is equal to 1, right?
So when t equals 0, this function is equal to A.
So this function probably looks something like A cosine
of-- and I'll just use the variable omega t-- it probably
looks something like that, this function.
And we'll learn in a second that it looks
exactly like that.
But I want to prove it to you, so don't just
take my word for it.
So let's just figure out how we can figure out what w is.
And it's probably a function of the mass of this object and
also probably a function of the spring
constant, but I'm not sure.
So let's see what we can figure out.
Well now I'm about to embark into a little bit of calculus.
Actually, a decent bit of calculus.
And we'll actually even touch on differential equations.
This might be the first differential equation you see
in your life, so it's a momentous occasion.
But let's just move forward.
Close your eyes if you don't want to be confused, or go
watch the calculus videos at least so you know what a
derivative is.
So let's write this seemingly simple equation, or let's
rewrite it in ways that we know.
So what's the definition of force?
Force is mass times acceleration, right?
So we can rewrite Hooke's law as-- let me switch colors--
mass times acceleration is equal to minus the spring
constant, times the position, right?
And I'll actually write the position as a function of t,
just so you remember.
We're so used to x being the independent variable, that if
I didn't write that function of t, it might get confusing.
You're like, oh I thought x is the independent variable.
No.
Because in this function that we want to figure out, we want
to know what happens as a function of time?
So actually this is also maybe a good review
of parametric equations.
This is where we get into calculus.
What is acceleration?
If I call my position x, my position is equal to x as a
function of t, right?
I put in some time, and it tells me what my x value is.
That's my position.
What's my velocity?
Well my velocity is the derivative of this, right?
My velocity, at any given point, is going to be the
derivative of this function.
The rate of change of this function with respect to t.
So I would take the rate of change with
respect to t, x of t.
And I could write that as dx, dt.
And then what's acceleration?
Well acceleration is just the rate of change
of velocity, right?
So it would be taking the derivative of this.
Or another way of doing it, it's like taking the second
derivative of the position function, right?
So in this situation, acceleration is equal to, we
could write it as-- I'm just showing you all different
notations-- x prime prime of t, second derivative of x with
respect to t.
Or-- these are just notational-- d squared x over
dt squared.
So that's the second derivative.
Oh it looks like I'm running out of time.
So I'll see you in the next video.
Remember what I just wrote. just wrote