Parametric to Polar Conversion

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Homework Help Overview

The discussion revolves around converting parametric equations of the form x=x(t) and y=y(t) into a polar equation r=r(θ). Participants explore the relationships between Cartesian and polar coordinates, particularly focusing on the conversion process and the implications of eliminating the parameter t.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • One participant attempts to eliminate the parameter t by solving for t in terms of x and substituting into y, questioning the validity of this method and whether it can be done without inverting the function. Others discuss the implications of this approach, particularly regarding the existence of inverses for certain functions.
  • Another participant provides an example of eliminating t and converting to polar coordinates, while also noting a useful conversion formula involving θ.
  • A different participant mentions the absence of the parametric equations and expresses a desire to derive them from a differential equation, indicating a shift in focus from conversion to formulation.

Discussion Status

The discussion is active, with participants sharing different perspectives on the conversion process and the challenges involved. Some guidance has been offered regarding the elimination of t and the use of polar coordinates, while multiple interpretations of the problem are being explored. There is no explicit consensus, but productive dialogue is ongoing.

Contextual Notes

One participant notes a lack of formal education in calculus, which may influence their understanding of the mathematical concepts being discussed. Additionally, there is a mention of a differential equation that is being reformulated in terms of θ, indicating a specific context for the problem.

Zach Knight
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Homework Statement


Convert the two equations x=x(t) and y=y(t) to a polar equation of the form r=r(\theta)


Homework Equations


x=r*cos(\theta)
y=r*sin(\theta)
r^{2}=x^{2}+y^2


The Attempt at a Solution


Perhaps I'm over-thinking this, but in order to eliminate the parameter t, I solved one of the two parametric equations, say x(t), for t, giving an equation t=t(x). I then substituted this equation into y(t), giving y=y(t(x)). Afterward, I used the identities listed above to convert y to r. Is this valid? Is there a way to do this without having to invert one of the functions?
 
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Zach Knight said:

Homework Statement


Convert the two equations x=x(t) and y=y(t) to a polar equation of the form r=r(\theta)


Homework Equations


x=r*cos(\theta)
y=r*sin(\theta)
r^{2}=x^{2}+y^2


The Attempt at a Solution


Perhaps I'm over-thinking this, but in order to eliminate the parameter t, I solved one of the two parametric equations, say x(t), for t, giving an equation t=t(x). I then substituted this equation into y(t), giving y=y(t(x)). Afterward, I used the identities listed above to convert y to r. Is this valid? Is there a way to do this without having to invert one of the functions?
It doesn't seem valid to me. For one thing, when you solve for t in terms of x, you are finding the inverse of the original function, which may or may not exist. For example, if x = f(t) = t2 + 3, f is not one-to-one, so doesn't have an inverse.

The usual approach is to eliminate the parameter t, and then replace x and y using the identities you show.

For example, if x = t and y = t2, x2 - y = t2 - t2 = 0,
so r2cos2(theta) - rsin(theta) = 0.

This is equivalent to rcos2(theta) - sin(theta) = 0, or r = sin(theta)/cos2(theta), so here we have r as a function of theta. Eliminating one factor of r is legitimate in this case since there is at least one value of theta for which sin(theta)/cos2(theta) = 0 (namely theta = 0, and others), so we haven't lost any solutions by getting rid of the factor of r.

There is one conversion formula that you didn't show, that is sometimes useful: theta = tan-1(y/x).
 
But where are your parametric equations you want to convert to polar coordinates? x= rcos(\theta) and y= r sin(\theta) are NOT parametric equations- they are true for all points in the plane.
 
The thing is, I don't have the parametric equations; I'm trying to find them via a differential equation. I'm trying to formulate
\frac{d^2\vec{r}}{dt^2}=\frac{-MG}{|r|^3}\vec{r}
in terms of \theta because the only way I could find to solve the above equation was to assume |r| was a constant. I think I have it now though. I rewrote the problem in terms of the unit vector
\hat{r}=cos(\theta)\hat{i}+sin(\theta)\hat{j}
and got
(\frac{d^2r}{dt^2}-r(\frac{d\theta}{dt})^2)\hat{r}+(2\frac{dr}{dt}\frac{d\theta}{dt}+r\frac{d^2\theta}{dt^2})\frac{d\hat{r}}{dt} = \frac{-MG}{r^2}\hat{r},
a differential equation I think I can actually solve.
Sorry if any of the math or notation is wrong; I haven't had a calculus class yet, so my education isn't very formalized yet.
 

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