Why Use a Trigonometric Substitution for a Free-Fall Problem?

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SUMMARY

The discussion focuses on the application of trigonometric substitution in solving a free-fall problem where gravitational force varies with height. The initial conditions are defined by total energy E, and the solution involves integrating the velocity function derived from conservation of energy. The key substitution used is cos(θ) = √(-Ex/mMG), which simplifies the integral necessary for finding the position as a function of time. Participants emphasize the importance of understanding the rationale behind this substitution to effectively solve similar integrals.

PREREQUISITES
  • Understanding of classical mechanics, specifically free-fall dynamics.
  • Familiarity with conservation of energy principles in physics.
  • Knowledge of integral calculus, particularly techniques for solving definite integrals.
  • Experience with trigonometric identities and substitutions in calculus.
NEXT STEPS
  • Study the derivation of gravitational force equations, particularly F = -mMG/x^2.
  • Learn about conservation of energy in variable gravitational fields.
  • Explore trigonometric substitution techniques in integral calculus.
  • Practice solving integrals involving du/(1-u^2) using trigonometric identities.
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Students of physics, mathematicians, and educators seeking to deepen their understanding of trigonometric substitutions in calculus, particularly in the context of mechanics and free-fall problems.

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Problem background:
  • Body free-falling towards the earth.
  • Account for variation in gravitational force with height.
  • Neglect air resistance.
  • Initial conditions summarized by total energy E.

I'm having trouble understanding part of my textbook's solution to this problem, so I will paraphrase said solution up until I have trouble. My comments are in bold.

Beginning with

[tex]F=-\frac{mMG}{x^2}[/tex],​

it can be shown that

[tex]V(x)=-\frac{mMG}{x}[/tex].​

By application of conservation of energy, we determine

[tex]v=\frac{dx}{dt}=\sqrt{\frac{2}{m}}\left[E-V(x)\right]^\frac{1}{2}=\sqrt{\frac{2}{m}}\left[E+\frac{mMG}{x}\right]^\frac{1}{2}[/tex].​

In order to find x(t), we must evaluate

[tex]\int^x_{x_0}\frac{dx}{\left(E+\frac{mMG}{x}\right)^\frac{1}{2}}=\sqrt{\frac{2}{m}}t[/tex].​

I can easily follow the math up to this point, but the next step in the textbook solution throws me off.

To solve the case when E is negative, substitute

[tex]\cos{\theta}=\sqrt{\frac{-Ex}{mMG}}[/tex],​

and we arrive at

[tex]\frac{mMG}{\left(-E\right)^\frac{3}{2}}\int^\theta_{\theta_0}2\cos^2\theta d\theta=\sqrt{\frac{2}{m}}t[/tex].​

If I assume this substitution to be valid, I can easily follow the rest of the textbook to the solution. However, where does this seemingly random substitution come from? And can anyone show how it is mathematically applied to the integral? I don't feel right blindly accepting the trig substitution and would appreciate clarification.

Thanks
 
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Because you say E is negative ==> -E > 0.

Lets consider:

[tex] \sqrt{E + \frac{mMG}{x}} = \sqrt{(-E)(-1 + \frac{mMG}{-Ex}[/tex]

From this point, you should imagine that you need substitution to solve this integral. Usually, the best way to solve du/(1-u^2) is using trigonometry. You can try to put cos/sin(u) = sqrt(mMG\-Ex) and then using a substitution from your textbook you will find that which way is more better.

The more practice you do with this type of integral, the more sense you have when you find a best way, that's my exp.
 

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