Math 128, Modern Geometry
D. Joyce, Clark University
19 Oct 2005
Due Today. From Chapter 7: 1, 6, 9, 10.
Due Monday. From Chapter 8: 1, 2, 8.
Properties of distance. The important thing
about this dis
Math 128, Modern Geometry
D. Joyce, Clark University
25 Aug 2005
Theres more than one kind of geometry
You have probably only seen one kind of plane geometry so far, classical Euclidean geometry, but
Summary of basic probability theory, part 3
D. Joyce, Clark University
Math 218, Mathematical Statistics, Jan 2008
Joint distributions. When studing two related
real random variables X and Y , it is n
Summary of basic probability theory, part 1
D. Joyce, Clark University
Math 218, Mathematical Statistics, Jan 2008
9. If event E is a subset of event F , then P (E)
P (F ).
10. Statement 7 above is c
Common probability distributions
D. Joyce, Clark University
Aug 2006
1
Introduction.
I summarize here some of the more common distributions used in probability and statistics.
Some are more important
A short introduction to Bayesian statistics, part V
D. Joyce, Apr 2009
Normal distributions with unknown variances. Lets now consider normal distributions
with both unknown mean and unknown variance
A short introduction to Bayesian statistics, part IV
D. Joyce, Apr 2009
6
Normal distributions.
Thus, the family of all normal distributions is a
conjugate family for .
Example. Lets take an example.
A short introduction to Bayesian statistics, part III
D. Joyce, Apr 2009
5
The Poisson process
Gamma(, r). There are a couple dierent ways
that gamma distributions are parametrizedeither
in terms of a
A short introduction to Bayesian statistics, part II
D. Joyce, Apr 2009
Bayes pool table example. The process we
just completed is what Thomas Bayes (17021761)
did. He illustrated the problem with bal
A short introduction to Bayesian statistics, part I
D. Joyce, Apr 2009
2nk
2nk + 2k
P (B|X) = 1 P (A|X)
2k
= nk
2
+ 2k
Ill try to make this introduction to Bayesian
statistics clear and short. First w
Example 1 (A radial vector eld). Well look as
several vector elds in the plane, and draw them
by drawing a few vectors F(x) with their tails attached to the points x. For instance, the vector
eld F(x)
speed, x , to be the length of velocity, so speed is
a nonnegative scalar.
So, at a time t, an object has a position x = x(t);
a velocity x = x (t), which is sometimes denoted
v = v(t); an acceleratio
is a good approximation of f near a in the sense
that
f (x) h(x)
= 0.
lim
xa
xa
Note that when m = 1, this denition says the
derivative Df of the scalar-valued function f is the
1 n row-matrix
Total d
A Lorenz attractor. Math 131 Multivariate Calculus
D Joyce, Spring 2014
A Lorenz attractor. Sometimes surprising things can happen. Lets start with this vector
eld in space.
8
F(x, y, z) = (10(y x), 2
Note how y and z dont change in this limit.
This kind of derivative is called a partial derivative since only one of the variables changes. Furthermore, the concept of limit used here is just the
Part
Whereas a line is parametrized by one variable
weve usually used ta surface is parametrized by
two variableswell usually use s and t.
It helps to have a standard notation. Well use S
to denote the sur
Surface integrals
Math 131 Multivariate Calculus
D Joyce, Spring 2014
The area dierential of a surface, and a double integral for the area of the surface.
Recall that were using X(s, t) to describe a
Theorem 1. When the rst and second partials of
a function of two variables x and y are all continuous functions, the order that the partials are taken
doesnt matter, that is, fyx = fxy , or in partial
About some topological concepts. In the
text theres a discussion of various topological
conceptsopen, closed, boundary, neighborhood,
and accumulation point. These are particularly important when the
the standard (x, y, z ) coordinate three-space. Notations for vectors. Geometric interpretation as vectors as displacements as well as vectors as points.
Vector addition, the zero vector 0, vector sub
and its derivative is the acceleration,
a(t) = v = x = (x , y , z ).
Now, Kepler determined that the acceleration of
the planet was toward the sun. Newton explained
that in terms of gravitational forc
Now lets add limits of integration. If the limits
of integration for u are a and b, then the limits of
integration for x will be x(a) and x(b).
x(b)
Jacobians
Math 131 Multivariate Calculus
b
f (x) dx
system mentioned above has these three equations
fx (x, y ) = 2y = gx (x, y ) = 2x
fy (x, y ) = 2x + 2y = gy (x, y ) = 2y
g (x) = x2 + y 2 = c = 1
Lagrange multipliers
Math 131 Multivariate Calculus
i
Gradients
Math 131 Multivariate Calculus
D Joyce, Spring 2014
f
Last time. Introduced partial derivatives like
x
of scalar-valued functions Rn R, also called
scalar elds on Rn .
Total derivatives. Wev
Onto functions (surjective), one-to-one functions (injective), one-to-one correspondences
(bijective), range. These terms mean the same
thing in multivariate calculus as they in calculus of
a single v
D
M
dA as follows.
y
M
dA
y
D
b
(x)
M
dy dx
y
a
(x)
Proof of Greens theorem
Math 131 Multivariate Calculus
=
D Joyce, Spring 2014
(x)
b
M (x, y)
=
a
Summary of the discussion so far.
b
M (x, (x) M (x
Here, the symbol is just a variant of thats often
used for line integrals when the line is a closed curve
or a nite union of closed curves.
Greens theorem
Math 131 Multivariate Calculus
Example 1. Let
The surface x2 + y 2 + 1 = z is a paraboloid opening
upward (positive z being upward) with vertex on
the z -axis at z = 1. Above that surface and below
the plane z = 5 lies the 3-dimenional region D.
If the second derivative f (a) was 0, then you had
to try some other way to determine whether it
was a max or min or neither. We need some sort
of second-derivative test for the multidimensional
case.