What is the Length of a Parabolic Segment Using Calculus 3?

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Homework Help Overview

The problem involves finding the length of a parabolic segment defined by the polar equation r = 12/(1 + cos(θ)) over the interval 0 ≤ θ ≤ π/2. The context is rooted in calculus, specifically in the application of integrals to determine arc length.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the integral setup for calculating the length, with attempts to simplify the integrand using trigonometric identities. Some express confusion about the integration process and the use of reduction formulas.

Discussion Status

The discussion is ongoing, with participants sharing various approaches and expressions for the integral. Some have provided partial results and insights into potential simplifications, while others are questioning their calculations and the correctness of their methods.

Contextual Notes

There are indications of confusion regarding the correct application of trigonometric identities and integration techniques. Participants are also navigating through the complexities of the integral, with some expressing uncertainty about the outcomes from computational tools.

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Homework Statement



Find the length of the parabolic segment r = [itex]\frac{12}{1+cos(θ))}[/itex], 0[itex]\leq[/itex]θ[itex]\leq[/itex][itex]\frac{∏}{2}[/itex].

Homework Equations



L = ∫[itex]\sqrt{f(θ)^{2}+f^{'}(θ)^{2}}[/itex]dθ

The Attempt at a Solution



I got up to here and didn't know whta to do

L = 12 [itex]∫^{0}_{\frac{∏}{2}}[/itex] [itex]\frac{1}{1+cos(θ)}[/itex][itex]\sqrt{1+(\frac{sin(θ)}{1+cos(θ)})^{2}}[/itex]dθ

Wolfram alpha doesn't know neither

[itex]f(θ)^{2}[/itex] = [itex](\frac{12}{1+cos(θ))})^{2}[/itex]
[itex]f^{'}(θ)^{2}[/itex] = [itex](\frac{12sin(θ)}{(1+cos(θ))^{2}})^{2}[/itex]
[itex]\sqrt{f(θ)^{2}+f^{'}(θ)^{2}}[/itex] = [itex]\sqrt{(\frac{12}{1+cos(θ))})^{2}+(\frac{12sin(θ)}{(1+cos(θ))^{2}})^{2}}[/itex]=[itex]\frac{12}{1+cos(θ)}\sqrt{1+(\frac{sin(θ)}{1+cos(θ)})^{2}}[/itex]
 
Last edited:
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GreenPrint said:

Homework Statement



Find the length of the parabolic segment r = [itex]\frac{12}{1+cos(θ))}[/itex], 0[itex]\leq[/itex]θ[itex]\leq[/itex][itex]\frac{∏}{2}[/itex].

Homework Equations



L = ∫[itex]\sqrt{f(θ)^{2}+f^{'}(θ)^{2}}[/itex]dθ

The Attempt at a Solution



I got up to here and didn't know whta to do

L = 12 [itex]∫^{0}_{\frac{∏}{2}}[/itex] [itex]\frac{1}{1+cos(θ)}[/itex][itex]\sqrt{1+(\frac{sin(θ)}{1+cos(θ)})^{2}}[/itex]dθ

Wolfram alpha doesn't know neither
Mod note: Fixed incorrect = in the identity below.[/color]
First, simplify the integrand using trig identities such as [itex]\sin^2(\theta) + \cos^2(\theta) = 1.[/itex] After that, Maple manages to do the integral, but I won't report the answer here: you can try again after simplification, substitution, etc. BTW: to get [itex]\int_{0}^{\pi/2}[/itex] you need to type \int_{0}^{\pi/2}, not what you typed.

RGV
 
Last edited by a moderator:
oh hm ok thanks i got to go ill be back later
 
well i tired to simplify it further but keep on getting stuck

12 square root (2) * integral[0,pi/2] d theta/(sin(theta)+sin(2*theta))

is as far as i got
 
I entered a approximation into the answer box and it told me i was wrong so i guess it wants a exact answer

here is what it said (see attachment) I'm not sure it really helps

also note that I tried to evaluate
12 square root (2) * integral[0,pi/2] d theta/(sin(theta)+sin(2*theta))
using trig substitution with angle alpha
cot(alpha)^2/2 = cos(theta)
I would have to solve for theta
and then find d theta/ d alpha
solve for d alpha
and use the fact that
cos(alpha)^2/sin(theta) = 1/(sin(theta)+sin(2theta))
but I'm not sure if this will all work

i believe that it's equivalent
that is 12 square root (2) * integral[0,pi/2] d theta/(sin(theta)+sin(2*theta))
 

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So here is were I'm at now

L = 12 [itex]∫^{\frac{∏}{2}}_{0}[/itex] [itex]\frac{1}{1+cos(θ)}[/itex][itex]\sqrt{1+(\frac{sin(θ)}{1+cos(θ)})^{2}}[/itex]dθ

from here I used the fact that
1 + cos(θ) = 2[itex]cos^{2}[/itex]([itex]\frac{θ}{2}[/itex])
so
[itex]\frac{sec^{2}(\frac{θ}{2})}{2}[/itex] = [itex]\frac{1}{1+cos(θ)}[/itex]
similarly
[itex]\sqrt{1+(\frac{sin(θ)}{1+cos(θ)})^{2}}[/itex] = [itex]\sqrt{1+\frac{sec^{4}(\frac{θ}{2})sin^{2}(θ)}{4}}[/itex]
So I know have the following

L = 12 [itex]∫^{\frac{∏}{2}}_{0}[/itex] [itex]\frac{1}{1+cos(θ)}[/itex][itex]\sqrt{1+(\frac{sin(θ)}{1+cos(θ)})^{2}}[/itex]dθ = 12 [itex]∫^{\frac{∏}{2}}_{0}[/itex] [itex]\frac{sec^{2}(\frac{θ}{2})}{2}[/itex] [itex]\sqrt{1+\frac{sec^{4}(\frac{θ}{2})sin^{2}(θ)}{4}}[/itex]dθ
from here I use the fact that
[itex]sin^{2}[/itex](θ)=4[itex]sin^{2}[/itex]([itex]\frac{θ}{2}[/itex])[itex]cos^{2}[/itex]([itex]\frac{θ}{2}[/itex])
wolfram alpha confirm it's true
http://www.wolframalpha.com/input/?i=sin(x)^2=4sin(x/2)^2*cos(x/2)^2
plugging this in I get

12 [itex]∫^{\frac{∏}{2}}_{0}[/itex] [itex]\frac{sec^{2}(\frac{θ}{2})}{2}[/itex] [itex]\sqrt{1+sec^{4}(\frac{θ}{2})sin^{2}(\frac{θ}{2})cos^{2}(\frac{θ}{2})}[/itex]dθ=6 [itex]∫^{\frac{∏}{2}}_{0}[/itex] [itex]sec^{2}(\frac{θ}{2})[/itex][itex]\sqrt{1+sec^{2}(\frac{θ}{2})sin^{2}(\frac{θ}{2})}[/itex]dθ, u = [itex]\frac{θ}{2}[/itex], [itex]\frac{du}{dθ}[/itex]=[itex]\frac{1}{2}[/itex],du=[itex]\frac{dθ}{2}[/itex],dθ=2du,L=12 [itex]∫^{θ=\frac{∏}{2}}_{θ=0}[/itex] [itex]sec^{2}(u)[/itex][itex]\sqrt{1+sec^{2}(u)sin^{2}(u)}[/itex]du=12 [itex]∫^{θ=\frac{∏}{2}}_{θ=0}[/itex] [itex]sec^{2}(u)[/itex][itex]\sqrt{1+tan^{2}(u)}[/itex]du
then from here I use
[itex]sin^{2}(θ)[/itex])+[itex]cos^{2}(θ)[/itex]=1
that if I divide through by [itex]cos^{2}(θ)[/itex] I get
[itex]tan^{2}(θ)[/itex])+1=[itex]sec^{2}(θ)[/itex]
L=12 [itex]∫^{θ=\frac{∏}{2}}_{θ=0}[/itex] [itex]sec^{2}(u)[/itex][itex]\sqrt{sec^{2}(u)}[/itex]du=12[itex]∫^{θ=\frac{∏}{2}}_{θ=0}[/itex] [itex]sec^{3}(u)[/itex]du
then because
∫[itex]sec^{n}(x)dx = \frac{sec^{n-2}(x)tan(x)}{n-1}+\frac{n-2}{n-1}∫sec^{n-2}(x)dx[/itex]
we got
12[itex]∫^{θ=\frac{∏}{2}}_{θ=0}[/itex] [itex]sec^{3}(u)du=12[\frac{sec(u)tan(u)}{2}+\frac{1}{2}∫sec(u)du]|^{θ=\frac{∏}{2}}_{θ=0}[/itex]
and because
∫sec(x)dx=ln|sec(x)+tan(x)|+c
we got
[itex]12[\frac{sec(u)tan(u)}{2}+\frac{1}{2}∫sec(u)du]|^{θ=\frac{∏}{2}}_{θ=0}=12[\frac{sec(u)tan(u)}{2}+\frac{1}{2}ln(|sec(u)+tan(u)|)]|^{θ=\frac{∏}{2}}_{θ=0}[/itex]
plugging back in
u = [itex]\frac{θ}{2}[/itex]
we got
[itex]12[\frac{sec(u)tan(u)}{2}+\frac{1}{2}ln(|sec(u)+tan(u)|)]|^{θ=\frac{∏}{2}}_{θ=0}=12[\frac{sec(\frac{θ}{2})tan(\frac{θ}{2})+ln|sec(θ/2)+tan(\frac{θ}{2})|}{2}]|^{θ=\frac{∏}{2}}_{θ=0}=12[\frac{sec(\frac{∏}{4})tan(\frac{∏}{4})+ln(|sec(∏/4)+tan(\frac{∏}{4})|)}{2}-\frac{sec(0)tan(0)+ln(|sec(0)+tan(0)|}{2})=12[\frac{\sqrt{2}+ln(|\sqrt{2}+1|)}{2}-0][/itex]=6([itex]\sqrt{2}[/itex]+ln([itex]\sqrt{2}+1)[/itex])
 
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I haven't worked the problem through, but here is what I got.

r2 + (r')2 = [tex]\frac{288}{(1 + cosθ)^3}[/tex]

You still need to take the square root, and then integrate that result. No doubt another trig identity will come in useful.
 
I have no idea how you got that. I get

[itex]\frac{144}{(1+cos(θ))^{2}}[/itex] + [itex]\frac{144(1-cos^{2}(θ))}{(1+cos(θ))^{4}}[/itex] = [itex]\frac{144}{(1+cos(θ))^{2}}(1+[/itex][itex]\frac{1-cos^{2}(θ)}{(1+cos(θ))^{2}}[/itex])

when I try to expand it
 
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well i found one mistake in my work i forgot to square the two let's see...
 
  • #10
GreenPrint said:
I have no idea how you got that. I get

[itex]\frac{144}{(1+cos(θ))^{2}}[/itex] + [itex]\frac{144(1-cos^{2}(θ))}{(1+cos(θ))^{4}}[/itex] = [itex]\frac{144}{(1+cos(θ))^{2}}(1+[/itex][itex]\frac{1-cos^{2}(θ)}{(1+cos(θ))^{2}}[/itex])

when I try to expand it

In the first line above, 1 - cos2θ = sin2θ, right?
 
  • #11
yes...
if you see I believe I had the right answer above... I actually got an answer which is a improvement...
I got the integral of sec^3(x) dx
but I get the wrong answer did I use the wrong reduction formula or something =( I think it's the right reduction formula but I'm not sure
 
  • #12
ok well i did use the right reduction formula
at first i had tan(pi/4)=sqrt(2)/2 but it's one i fixed that and updated my answer above
I don't see what I've done wrong but apparently it is
my calculator gives me 13.77735
and when i put in the answer i got i get 7.4787
 
  • #13
I checked what I had in wolframalpha, and got 13.7735 (two 7's, not 3), which sort of agrees with your calculator answer.

You have a ton of stuff in post #6, too much to wade through to find an error.

The integral should look like this, if my work is correct:
[tex]12\sqrt{2}\int_0^{\pi/2} \frac{d\theta}{(1 + cos\theta)^{3/2}}[/tex]

There's a half-angle identity that might be useful here: cosθ + 1 = 2 cos2(θ/2). This turns the integral above into
[tex]12\sqrt{2}\int_0^{\pi/2} \frac{d\theta}{(2^{3/2}cos^3(\theta/2))}[/tex]

Then it should be a relatively simple matter of integrating sec3 of something. There's a wikepedia page on this integral.
 
  • #14
ya the only problem is that i don't think there is an error in my work i have checked over it a lot, it's not as long as it seems it's just that I showed each step and my reasoning and any formulas I used, I included the reduction formula for integrating secant
I got it down to
12 integral sec^3(u) du

similar to what you got
6*sqrt(2) integral sec^3(x)
interesting enough when i enter this into my calculator with limits i get divide by zero error :O when i try to put in what you got 12*sqrt(2)*integral[0,pi/2] sec^3(x)dx
and wolfram alpha
http://www.wolframalpha.com/input/?...t(2)*integral[0,pi/2]+sec^3(x)dx&incTime=true
couldn't give an approximation or exact answer
hmm...
 
  • #15
it told me that the correct answer is
6*(sqrt(2)+ln(1+sqrt(2))
yay i got it right and found my error yippeeee
 
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