How Are Polar and Cartesian Graphs of \( r = e^{\theta} \) Related?

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SUMMARY

The discussion centers on the relationship between the polar graph of \( r = e^{\theta} \) and the Cartesian graph defined by the parametric equations \( x = \theta \cos{\theta} \) and \( y = \theta \sin{\theta} \). The user attempts to establish a connection by equating \( e^{2\theta} \) with \( \theta^2 \) and finds that the equation \( e^{\theta} = \theta \) has no real solutions, indicating that the graphs intersect at points where \( e^{\theta} = -\theta \). The conversation highlights the significance of plotting the curves to visualize their intersections and suggests that successive derivatives of \( r = e^{\theta} \) lead to a tighter spiral, ultimately relating to trigonometric functions.

PREREQUISITES
  • Understanding of polar coordinates and their equations
  • Familiarity with Cartesian coordinates and parametric equations
  • Knowledge of exponential functions and logarithms
  • Basic calculus concepts, including derivatives
NEXT STEPS
  • Explore the relationship between exponential functions and trigonometric functions through Euler's formula
  • Learn about numerical methods for finding roots of equations, such as the Newton-Raphson method
  • Investigate the properties of polar curves and their derivatives
  • Study the graphical representation of polar and Cartesian equations to understand their intersections
USEFUL FOR

Mathematics students, educators, and anyone interested in the connections between polar and Cartesian graphs, particularly in the context of exponential and trigonometric functions.

gordonj005
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Homework Statement



"Consider the graph of r = e^{\theta} in polar coordinates. Then consider the graph of (\theta \cos{\theta}, \theta \sin{\theta}) where \theta \in \mathbb{R} on the Cartesian plane (x - y axis). How are the two graphs related? What relationship (if any) can we define between e^{\theta} and the trigonometric functions?

The Attempt at a Solution



What I considered was r^2 = x^2 + y^2 where x = \theta \cos{\theta} and y = \theta \sin{\theta}. Plugging this all in I get:

e^{2\theta} = (\theta)^2 ((\cos{\theta})^2 + (\sin{\theta})^2)

which reduces to:

e^{2 \theta} = (\theta)^2

taking the ln of both sides, noting that \theta \ne 0:

2 \theta = 2 ln \theta

\theta = ln \theta

So as it stands now, the above equation has no real solutions. So I thought maybe putting each side as a power of e would be the relation between the two graphs.

e^{\theta} = e^{ln \theta}

e^{\theta} = {\theta}

which is kind of a circluar argument because I just rearranged the equation. They mention this has something to do with trigonometric functions, I'm not seeing the connection. I would apprectiate some help.
 
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What you have done is define two equations, r^2 = \theta^2 and r = e^\thetaand then solve them simultaneously. The value of θ satisfying e^\theta = \thetais simply where the two graphs intersect.
 
Yes, I realize this, but there are no real solutions to that equation. And also it doesn't tell me much about the relation between the two functions.
 
I have no idea about the rest of the problem, but I can tell you one thing. The curves do intersect. Just plot them. Show there is a solution to exp(t)=t+2*pi. You can find the root numerically if you want. Call it c. Now put c into the exponential and c+2*pi into the other curve. You'll get the same x,y coordinates. There are an infinite number of other similar solutions.
 
Last edited:
Oops, I omitted the negative sign! e^\theta = \theta has no real roots, but e^\theta = -\theta does!
 
Ah right you are, I thought that seemed weird that there were real intersection points but no solution. One thought i had was that if you take successive derivatives of r = e^{\theta} you will get a tighter and tigher spiral. Eventually you should get the parametric function: (\theta \cos{\theta}, \theta \sin{\theta}). Any thoughts?
 
I've seen that before, its very nice. But does it have an application here?
 
gordonj005 said:
Ah right you are, I thought that seemed weird that there were real intersection points but no solution. One thought i had was that if you take successive derivatives of r = e^{\theta} you will get a tighter and tigher spiral. Eventually you should get the parametric function: (\theta \cos{\theta}, \theta \sin{\theta}). Any thoughts?

Derivatives with respect to what? That doesn't sound right. I still don't quite get the point of this problem, I share that with you.
 
  • #10
Derivatives with respect to \theta. I'm not sure, at this point I'm just grasping at answers. Any other thoughts?
 

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