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Youwen Wu 2025-03-03 00:43:59 -08:00
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@ -1106,5 +1106,63 @@ Any 3D shape can be built recursively of atomic objects.
Schley what are you doing??? Schley what are you doing???
== Signed area and volume = Double integrals and some fun
We consider various types of integrals. Consult
#link("https://web.evanchen.cc/textbooks/poster-ints.pdf")[this chart] to
classify them.
Namely, we consider integrals of 0, 1, 2, and 3 dimensions, on scalar valued
function from $RR^0 -> RR$, $RR^1 -> RR$, $RR^2 -> RR$, and $RR^3 -> RR$.
To evaluate double integrals, we need to place notable importance on the
_region_ we integrate over.
== Integrating over rectangles
Integrating over a rectangle is super easy. It's like partial derivatives,
where we hold every other variable constant and integrate over our desired
value.
#example[
Evaluate
$ integral^6_0 integral^1_0 x y^2 dif x dif y $
We just crunch the numbers.
The first integral:
$
integral_0^1 x y^2 dif x = lr(1/2 x^2 y^2 |)_(x=0)^(x=1) = 1 / 2 y^2
$
The second integral:
$
integral_0^6 1 / 2 y^2 dif y = lr(1/6 y^3 |)_(y=0)^(y=6) = 36
$
]
== $x y$ integration without a rectangle
In general most 2D regions $cal(R)$ can still be done with $x y$ integration even when they aren't rectangles. In that case, we use the notation
$
integral.double_cal(R) f(x,y) dif x dif y := "integral of" f "over" cal(R)
$
If the region is given by inequalities, for instance, a unit disk, we would write
$
integral.double_(x^2 + y^2 <= 1) f(x,y) dif x dif y
$
== Swapping the order of integration
If our function is nice, then this is easy.
#theorem[Fubini's][
If the function that defines our surface is continuous, the double integral
over a rectangle can be evaluated in either order without a change to the
integral.
]
Otherwise, we want to swap the order of integration. We convert the limits of
integration back into inequality/region format, getting a region $cal(R)$ like
discussed in the previous section. Then evaluate that integral using standard
methods.

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@ -2261,7 +2261,7 @@ They are "easy" to use for finding the distributions of:
E[X^k] = mu_k, k = 1,2,... E[X^k] = mu_k, k = 1,2,...
$ $
Then the *moment generating function* of a random variable $X$ is defined by Then the *moment generating function* of a random variable $X$ is defined by
$M_x(t) = E[e^(t x)]$, for the real variable $t$. $M_x (t) = E[e^(t x)]$, for the real variable $t$.
] ]
All of the moments must be defined for the MGF to exist. The MGF looks like All of the moments must be defined for the MGF to exist. The MGF looks like