Equal Area Property of Ellipses: Proving A'(t) = (1/2)ab

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Discussion Overview

The discussion revolves around proving the derivative of the area swept out by an ellipse, specifically showing that A'(t) = (1/2)ab, where r(t) = . Participants explore the relationship between the area bounded by the polar curve and the angle Θ, engaging with concepts from calculus and trigonometry.

Discussion Character

  • Homework-related
  • Mathematical reasoning
  • Technical explanation
  • Exploratory

Main Points Raised

  • Some participants suggest using the chain rule to find A'(t) by relating it to A'(Θ) and Θ'(t).
  • There is uncertainty about the correct function for f(Θ) and whether to substitute Θ for t in r(t).
  • One participant expresses confusion regarding the integration process and the simplification of A'(Θ).
  • Another participant proposes that A'(Θ) can be directly equated to the function being integrated, prompting further discussion on this point.
  • Participants discuss the need to express trigonometric identities in terms of secant and tangent to simplify their equations.
  • There is a correction regarding the use of variables, with a participant clarifying the need to maintain consistency in using either t or Θ.
  • One participant identifies a potential error in their calculations related to the expressions for A'(Θ) and the use of trigonometric identities.
  • Another participant suggests that the area swept out by an angle Θ does not depend on the starting position, leading to a proposal for integrating A(Θ) over a specified interval.

Areas of Agreement / Disagreement

Participants express varying levels of understanding and approaches to the problem, with no consensus reached on the best method to prove A'(t) = (1/2)ab. Multiple competing views and methods are presented throughout the discussion.

Contextual Notes

Participants note the complexity of the integration process and the need for careful handling of trigonometric identities. There are unresolved questions about the assumptions made in the calculations and the definitions of the variables used.

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Homework Statement



Consider the ellipse r(t) = <acost, bsint>, for t between 0 and 2PI, where a and b are real numbers. Let Θ be the angle between the position vector and the x-axis.

a) Recall that the area bounded by the polar curve r = f(Θ) on the interval [0,Θ] is A(Θ) = (1/2) ∫ (f(u))^2 du, where in this case f(theta) = |r(Θ(t))|. Use this fact to show that A'(t) = (1/2)ab.


Homework Equations





The Attempt at a Solution

 
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hi physics_197! :wink:

Show us what you've tried, and where you're stuck, and then we'll know how to help! :smile:
 
tiny-tim said:
hi physics_197! :wink:

Show us what you've tried, and where you're stuck, and then we'll know how to help! :smile:

I'm not sure how to approach this problem to begin with. In earlier parts we were asked to show that tanΘ = (b/a)tan(t) and to find Θ'(t). I have those done and assume we will need to use them.

I have tried to integrate the function to find A(Θ). Then, to find A'(t), I though that I could use A'(Θ) * Θ'(t). I am not sure if that will work.

Also, I am not even sure I am using the correct function f(theta) = |r(Θ(t))|. I thought I could just plug Θ in for t for r(t) = <acost, bsint> to get r(Θ) = <acosΘ, bsinΘ> and then find the magnitude of that.
 
physics_197 said:
a) Recall that the area bounded by the polar curve r = f(Θ) on the interval [0,Θ] is A(Θ) = (1/2) ∫ (f(u))^2 du, where in this case f(theta) = |r(Θ(t))|. Use this fact to show that A'(t) = (1/2)ab.
physics_197 said:
… tanΘ = (b/a)tan(t) and to find Θ'(t).

I have tried to integrate the function to find A(Θ). Then, to find A'(t), I though that I could use A'(Θ) * Θ'(t). I am not sure if that will work.

you need to use the chain rule dA/dt = dA/dΘ dΘ/dt = dA/dΘ Θ'

(is that what you meant?)
Also, I am not even sure I am using the correct function f(theta) = |r(Θ(t))|. I thought I could just plug Θ in for t for r(t) = <acost, bsint> to get r(Θ) = <acosΘ, bsinΘ> and then find the magnitude of that.

yes that's correct …

carry on :smile:
 
When I tried that, I got a complicated answer (it may have simplified down to the correct answer). I was also wondering, Since we are told that A(theta) = the integral of another function, can we just say that A'(theta) = that function?
 
physics_197 said:
When I tried that, I got a complicated answer (it may have simplified down to the correct answer).

if you want us to check it, you'll have to write it out :wink:
I was also wondering, Since we are told that A(theta) = the integral of another function, can we just say that A'(theta) = that function?

yes, if A = ∫0t f(u) du, then dA/dt = f(t) :smile:
 
I got A'(theta) = (1/2)[ (acos(theta))2 + (bsin(theta))2 ] and Θ'(t) = (b/a)(sec(t))2 / (1 + (b/a tan(t) )2 )

After multiplying them and using some trig identities i got:

[ ab(1+(tant)2) + (b5/a3)(tant)2(1 + (tant)2) ]
---------------------------------------------
1 + ( (b/a) tant )2
 
you need to keep replacing b/a by tanΘ/tant

and to use one of the standard trigonometirc identities 1 + tan2 = sec2 :wink:

(get rid of all the coss and sins and tans, and replace them with sec and nothing else)
 
tiny-tim said:
you need to keep replacing b/a by tanΘ/tant

and to use one of the standard trigonometirc identities 1 + tan2 = sec2 :wink:

(get rid of all the coss and sins and tans, and replace them with sec and nothing else)

Have you worked it out? Because I am wondering if my equations are correct. Also, I understand what you are telling me, but I am having some trouble. Should I get everything in terms of t or theta? Other than what you mentioned before, are they any trig identities?
 
  • #10
physics_197 said:
Have you worked it out?

yes :smile:

start with a2cos2t + b2sin2t …

write that in terms of sect and secΘ without any cos or sin or tan :wink:
 
  • #11
tiny-tim said:
yes :smile:

start with a2cos2t + b2sin2t …

write that in terms of sect and secΘ without any cos or sin or tan :wink:

( a2cos2Θ + b2sin2Θ ) * [ (b/a)sec2t / sec2Θ ]

Then I get it to:

[ ( a2 + b2sec2Θ - b2 ) / sec2Θ ] * [ (b/a)sec2t / sec2Θ ]
 
  • #12
ah, now i see where you're going wrong …

where did you get that a2cos2Θ + b2sin2Θ from?

shouldn't it be a2cos2t + b2sin2t ?
 
  • #13
I thought it was theta because it is A'(Θ).

Using t, I get:

[ ( a2 + b2sec2t - b2 ) ] * [ (b / asec2Θ ]
 
Last edited:
  • #14
and b2sec2t - b2 = … ? :smile:
 
  • #15
tiny-tim said:
and b2sec2t - b2 = … ? :smile:

b2tan2t
But I am thinking your looking for something else.

EDIT: Never mind, it also equals a2tan2Θ

Thanks, got it now :)

The next part asks me to show that the area swept out by any angle theta is equal to the area swept out by the same angle (doesn't depend on where it starts).
I was thinking of integrating A(Θ) = (1/2) ∫ (f(u))^2 du over T to T+Θ where T is just some angle. And then somehow my answer will not have any T in it so I can clude that the area only depends on the angle swept out and not the starting position?
 
Last edited:
  • #16
hi physics_197! :smile:

(don't use T, it looks too much like t … use something like ψ or Θ0)

in the first part, you proved that dA/dΘ = ab/2,

so A(Θ) = abΘ/2,

and the area between Θ0 and Θ1 is ab(Θ1 - Θ0)/2 :wink:
 

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