Integrals, yay!
This one has a few parts :) Consider the function: \[\Gamma(x)=\int\limits_{0}^{infinity}t^{x-1}e^{-1}dt\] a) Find \[\Gamma(1), \Gamma(2)\] b) Integrate by parts to show that, for positive n, \[\Gamma(n+1)=n \Gamma(n)\] c) If n is a positive integer, find a much simpler expression for \[\Gamma(n)\]
So what is the issue?
Also, use `\infty` for \(\infty\).
oh thanks :D well..for part a) do I integrate and then plug the numbers in?
Woops, small typo in your gamma function,\[\large\rm \Gamma(x)=\int\limits\limits_{0}^{\infty}t^{x-1}e^{-t}dt\]But anyway, you plug in the value first, then integrate.\[\large\rm \Gamma(1)=\int\limits\limits\limits_{0}^{\infty}t^{1-1}e^{-t}dt\]
Would that 1-1 by the t just equal t^0 and did you mean e^{-1} ?
I meant e^{-t} that was your typo :o This is the Gamma Function, yes?
oh!! yes! Sorry, I was reading it all wrong. I thought the x by the t was a t. lol. Wait, let me restart haha
[eating dinner so a bit distracted. foood :>]
mm c:
ok so then it would be t^0
Yes, I suppose I should have said: ~Plug in the value ~Simplify* ~Integrate
okk xD em..so integration by parts?
No, not for this first one.
\[\large\rm \Gamma(1)=\int\limits_0^{\infty}t^0 e^{-t}dt=\int\limits_0^{\infty} e^{-t}dt\]
:o \[\Gamma(1)=e^{\infty}-e^{0}\]
oops those are negative ones
Negative, ya?\[\Gamma(1)=-\left[e^{\infty}-e^{0}\right]\]Btw, don't write that on your paper if you're handing it in :) Your teacher will not like you using infinity as a number lol
Rewrite it as an improper integral if it's something you have to hand in :P\[\large\rm \Gamma(1)=-\left[\lim_{b\to\infty}e^{-b}-e^0\right]\]
I dunno, maybe your teacher doesn't care :D lol
haha yeah i'll do that :) it's a project type thing so it must be most beautiful!! :D
so e^-inft = 0? and e^0 =1
Yes.
-[-1] = 1
\[\large\rm \Gamma(1)=1\]K cool, neeeeext.
\[\Gamma(2)=\int\limits_{0}^{\infty}t^1e^{-1}dt\]
bleeh ^-t on the e
\[\int\limits_{0}^{\infty}te^{-t}dt\] now integration by parts?
mhm
yay! gimme a moment :D
\[= te^{-t}-e^{-t}\]
evaluated from 0 to infty
u = t dv = e^-t
\[=- te^{-t}-e^{-t}\]
why is the first t negative?
Because uv is the first term. dv=e^{-t} v=-e^{-t}
\[=[(-\infty e^{-\infty}-e^{-\infty})-(-0e^{-0}-e^{-0})]\]
0-0-0-1 ?
0-0-0-(-1)
it = 1 too!
\[\large\rm \Gamma(2)=1\]Cool, next!
woowoo b)integrate by parts to show that, for positive n, gamma(n+1)=n(gamma)n
Mmm k, sounds simple enough.
\[\large\rm \Gamma(n+1)=\int\limits_0^{\infty}t^{n+1-1}e^{-t}dt\]
\[\int\limits_{0}^{t} t^n e^{-t}dt \]
u=t^n du = nt ?
or nt^{n-1}
ya
the second one?
yes one of those, ya let's go with the second lol
\[-t^n e^{-t}-\int\limits_{0}^{\infty}-e^{-t}*nt^{n-1}dt\]
k good.
uh so doing by parts again won't really help much.
Pull the negative and n out front,\[\large\rm -t^n e^{-t}+n\color{orangered}{\int\limits\limits_{0}^{\infty}t^{n-1}e^{-t}dt}\]What can we say about this orange thing?
It's super close to what we began with?
It sure is. It looks like the Gamma Function, but not G(n+1).
oooo because it's n(gamma)n it's n+1-1 so just n ?
Mmm good yes.\[\large\rm -t^n e^{-t}+n\color{orangered}{\Gamma(n)}\]Just need to show the other part is 0 at both boundaries, as you did similarly for G(2).
ah. So I evaluate the left of the + from 0 to infinity?
\[-t^n e^{-t} |^\infty_0+n \Gamma(n)\]
mhm
and once we plug those in it all just =0
Part next! :) last one c) if n is a positive integer, find a much simpler expression for Gamma(n)
...so do i plug n in for x?
I would solve the recurrence relation.
\[\Gamma(n+1)=n \Gamma(n) \\ \text{ with } \Gamma(1)=1 \ \ \text{ divide both sides of } \Gamma(n+1)=n \Gamma(n) \text{ by } \Gamma(n) \\ \frac{\Gamma(n+1)}{\Gamma(n)}= n\] Then take the product of both sides by from n=1 to n=k
you will see a lot of cancellation
on the left hand side
what what? @freckles
@freckles sorry, I was having a bit of a mini seizure. I just got accepted to the university I want to go to!! :) but now I am back hehe
Why would we set those equal to each other?
did you already do b?
That is where I got the equation from.
Yes we did b
\[\Pi_{n=1}^{k} \frac{\Gamma(n+1)}{\Gamma(n)}=\Pi_{n=1}^{k} n\]
I took the product of both sides
from n=1 to n=k
try simplifying both sides
I'm not sure what "taking the product" means? o.0
you can expand the products on both sides to see what is really happening
have you guys ever did sigma/sum thingys?
instead of adding you multiply in Pi/product thingys
Pi not being the number pi
Pi meaning product here
the E looking things? xD yeah
example right hand side is \[\prod_{n=1}^{k}n= 1 \cdot 2 \cdot 3 \cdot 4 \cdot 5 \cdots \cdot (k-1) \cdot k\]
which you can write as k!
try expanding the left hand side a bit
and you should see some really cool stuff happen
wait wait..trying to understand this heh
evaluate the thing we are taking the product of from n=1 to k=n and just multiply those results
just like you did with sums except we added
\[\Pi = \sum_{}^{}\] type thing?
no products aren't the same as sums in products we multiply in sums we add \[\sum_{i=1}^{3}(3i+5)= (3 \cdot 1+5)+(3 \cdot 2+5)+(3 \cdot 3+5) \\ \prod_{i=1}^{3}(3i+5)=(3 \cdot 1 +5)(3 \cdot 2+5)(3 \cdot 3+5)\]
oh I see o.o
I could have this without introducing that notation but chances are if you stick in math you will see that notation again
\[\frac{\Gamma(n+1)}{\Gamma(n)}=n\] So this is what we are trying to solve.... You already proved this equation in b So this means the following are true: \[\frac{\Gamma(2)}{\Gamma(1)}=1 \\ \frac{\Gamma(3)}{\Gamma(2)}=2 \\ \frac{\Gamma(4)}{\Gamma(3)}=3 \\ \frac{\Gamma(5)}{\Gamma(4)}=4 \\ \cdots \\ \frac{\Gamma(k)}{\Gamma(k-1)} =k-1 \\ \frac{\Gamma(k+1)}{\Gamma(k)}=k\]
this implies... \[\frac{\Gamma(2)}{\Gamma(1)} \cdot \frac{\Gamma(3)}{\Gamma(2)} \cdot \frac{\Gamma(4)}{\Gamma(3)} \cdot \frac{\Gamma(5)}{\Gamma(4)} \cdots \frac{\Gamma(k)}{\Gamma(k-1)} \cdot \frac{\Gamma(k+1)}{\Gamma(k)}=1 \cdot 2 \cdot 3 \cdot 4 \cdots (k-1) \cdot k\]
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