Calculus is one of the grandest achievements of human thought, explaining everything from planetary orbits to the optimal size of a city to the periodicity of a heartbeat. This brisk course covers the core ideas of single-variable Calculus with emphases on conceptual understanding and applications. The course is ideal for students beginning in the engineering, physical, and social sciences. Distinguishing features of the course include: 1) the introduction and use of Taylor series and approximations from the beginning; 2) a novel synthesis of discrete and continuous forms of Calculus; 3) an emphasis on the conceptual over the computational; and 4) a clear, dynamic, unified approach. In this fourth part--part four of five--we cover computing areas and volumes, other geometric applications, physical applications, and averages and mass. We also introduce probability.
Fair Probability
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From the course by University of Pennsylvania
Calculus: Single Variable Part 4 - Applications
ratings
From the lesson
An Introduction to Probability
This capstone module gives a very brief introduction to probability, using what we know about integrals and differential elements. Beginning with common-sense uniform probabilities, we move on to define probability density functions and the corresponding probability element. Building on the physical intuition obtained from centers of mass and moments of inertia, we offer a unique perspective on expectation, variance, and standard deviation.
Meet the Instructors
Robert GhristProfessor
Mathematics and Electrical & Systems Engineering
Welcome to calculus. I'm professor Griest.
We're about to begin lecture 42 on fair probability.
Lets take what we've learned about averages, moments, centroids, and put
them to use in an entirely different setting.
That of probability we're going to begin our introduction to probability with a
geometric treatment, that is both visual and visceral.
Our probability begins with counting. Consider something as simple as asking,
what happens when you roll a pair of dice?
What's the probability that the sum of the numbers you get adds to greater than
seven? Well, in this case, you can simply make a
table with all of the possible outcomes for the first and the second die.
Add up their face values and identify which of those are greater than 7.
When you do so, the probability is a ratio of the number of outcomes that are
greater than 7 to the total number of outcomes.
In this case, the numbers work out to 15 over 36.
That means you have to have a little bit less than a 50-50 chance of getting
something bigger than 7. Now, this is simple enough but do you see
an integral hiding in there somewhere. Stay tune.
Consider a simple situation of spinning a dial.
Some outcomes, you win, others you lose. You could compute the probability of a
win by counting sectors as before but there's another way to approach this.
One can think of the random variable as being an angle where some angles connote
a win. Spinning the dial corresponds to choosing
an angle at random between 0 and 2 pi. In this case, how would you compute the
probability? Well, one could think of it as a ratio
between the number of winning angles to the total number of angles.
But we're really not counting angles, are we?
We're really computing length in this simple example, one would get an answer
that is the same as counting segments. But in other examples, we would really
need to compute lengths. For example, what's the probability that
a randomly chosen angle on the circle has sine larger than one half.
Well, we would compute this probability as a ratio, as before.
The total number of angles has length to pi, the length of the circle.
If we look at those angles that have sine larger than one half, well, that length
is 2 pi over 3. Taking the ratio gives us a probability
of 1 3rd. We can do the same thing with area.
With what probability does a randomly chosen point in a square lie within the
inscribed circle. So, take the square, consider the
inscribed circle and then choose a point in the square at random.
Think of it as throwing a dart. What are the odds that you land inside
that circular region, well in this case it's going to be an area fraction.
We would take the area of the disc and divide by the area of the square that is
our probability. We can compute that easily enough if the
radius is r, than the disc has area pie r squared and the square has area 2r
quanity squared. That leads to pie over 4 or about 79%.
Those are your odds. In some context volume is the appropriate
tool. Consider the following, with what
probability does a randomly chosen point in a ball lie within the outer 1%.
That is within 1% of the boundary as measured by radius.
So, we have a solid ball radius r. It's the point that is chosen at random,
not the radius. Given a random point in that ball.
What are the odds that it's radial coordinate is within the outer 1%?
Well, we have to think in terms of volumes since this is a three dimensional
ball. We know the volume of a ball of radius r
is 4 3rds pie r cubed. So, to compute the probability in this
case, what kind of computation should we do?
Well, given our formula for volume, it's really easy to compute the volume of a
ball, if we pick a point at random in the ball, then the total volume of the
possibilities 4 3rds pi r cubed. Now, what are the odds that a randomly
chosen point lies within the inner 99%? Well, that too is a ball of radius .99 r.
And so, if you look at this fraction, this ratio of volumes this gives us the
odds of not being within the outer 1%. So, to compute the odds of being in the
outer 1%, we take one minus this ratio. What you'll notice is that there's some
convenient cancellation that goes on. The 4 3rd pi cancels.
And the r cubed cancel and we're left with 1 minus .99 cubed.
That works out to about .0297 et cetera, that means there's about a 3% probability
of being within that crust, that outer shell.
Notice, it's not 1% because it's the point that is random and not the radius.
Now, having done length, area, volume, of coarse, you know what's coming next.
That is, high dimensional volume or hypervolume.
In this case, let's repeat the problem with a ball of dimension n.
In this case, the volume of an n-dimensional ball, radius r, is some
constant v sub n times r to the n. You don't have to remember what that
constant v sub n is, because if we follow the exact same steps as before, computing
the probability of being within that outer 1%.
We get the ratio, the volume of that inner 99% ball, which is v sub n times
.99r to the nth, divided by the volume of the full n-dimensional ball v sub n r to
the n. Just as before the sub ends cancel, the r
to the n's cancel and we are left with 1 minus .99 to the n.
Now, what happens as n gets large, .99 to the n goes to 0.
And we're left with the somewhat surprising conclusion that when the
dimension is high enough, for example, if it is 459 or bigger then 99% of the
volume of this ball is in the crust. If you pick a point in the ball at
random, your odds of being within 1% of the boundary are greater than 99%.
That comes as a bit of a surprise. But not if you know how high dimensional
volume works. These examples illustrate the basis of
what we call fair probability or uniform probability.
For a uniform probability distribution over some domain D, whether it's a, a
ball or a circle or a square. Then, the probability of a random point
being in some subset A, within D is given by a fraction, by a volume fraction.
The probability of being within A is the ratio.
The volume of A to the volume of D. In this case, what we mean by volume is
dependent on the dimension. When we were spinning a dial, we looked
at length. When we were choosing a point at random
in the square, then we considered area fractions.
When we were choosing a point on a ball. Then, we were considering volume, either
three dimensional or higher, depending on the dimension of D.
And lastly, when we simply rolled dice, we were counting.
But that counting is in itself zero dimensional volume.
The volume associated to a discreet set. Now, that one example had some unique
features, in that there were two variables, that two die and they were
independent. And so we could compute probabilities in
terms of multiplication. For an example it involves both
independent variables and integrals. We're going to consider the classical
buffon needle problem. This problem goes as follows.
Consider a collection of parallel lines in the plane, separated by some distance,
l. Then drop a needle on the plane.
Let's say the needle also has length l. Then, what are the odds that you have a
crossing that the needle crosses one of the lines.
Well, one way to answer this question would be to drop a whole bunch of
needles, count how many of them crossed the line and divide by the total number
of needles that you dropped. That would be an approximation.
But we can do better that. If as stated, we let l denote the
distance between these parallel lines and the length of the needle, then what
variables do we use to characterize where a randomly tossed needle has fallen?
We'll let h denote the horizontal distance from the leftmost tip of the
needle to the rightmost, nearest line. But that doesn't completely characterize
the needle. We also need to know theta.
That is the angle that the needle makes with this line.
Now, what are the bounds on h and theta? H can vary between 0 and l.
Theta doesn't vary from 0 to 2 pi, but rather from 0 to pi by means of how we've
defined h in term of the left tip. Now, given this, how can we say, whether
or not, a needle crosses a line. Well, if we set up a right triangle based
on that needle, then the hypotenuse is of length l.
And we know the angle theta. Therefore, the horizontal width of this
triangle is equal to l times sine beta. If that quantity is greater than or equal
to h, then we have a crossing of the line.
So, if in this theta h plane we graph l times sine theta then, dropping a
collection of needles is the same thing as sampling this rectangle at random.
And any random point that obeys this inequality, that falls under the curve
can note a crossing. And now we can do some calculus because
these variables are independent. Changing h doesn't change theta, and
changing theta doesn't change h. Then we can compute the probability of a
crossing as an area fraction. In this case, taking the ratio of the
area under the curve to the total area of the rectangle.
What's the area under the curve? Why that's simply the integral.
This data goes from 0 to pi of l sin data D theta.
What's the area of the entire domain? It's the area of the rectangle, pi times
l. Now, I think you can do this integral in
your head noticing that the l's cancel, one obtains a probability of 2 over pi.
That's very interesting. But maybe more interesting than you might
suspect because of the following fact, this probability has pi within it.
And we have an interpretation in terms of dropping needles on say a sheet of paper.
This principle means that you should be able to approximate the value of pi
simply by dropping needles on a field of lines, counting how many times the needle
crosses the line. And then dividing by the total number of
needles that you dropped. That ratio should come closer and closer
to 2 over pi by taking the reciprocal, multiplied by 2.
You can, in principle, approximate pi. Maybe you should try it.
If you do, one of the things that you'll find is that probability is a somewhat
mysterious subject. You'll also learn a thing or two about
convergence. Our treatment of probability won't end
with volumes and needles and Pi. In fact, we've hardly begun.
In our next lesson, we're going to consider what happens when the world
isn't fair, or at least when the underlying probability distribution isn't
fair. To do that, we'll need to wed our
volumetric approach with a more mask based approach from our previous lessons.
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