Vertical projectile motion with quadratic drag (sign convention)

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SUMMARY

The discussion centers on solving problem number 2.38 from John R. Taylor's "Classical Mechanics," specifically addressing vertical projectile motion with quadratic drag. The user initially misapplied sign conventions in the equations of motion, leading to incorrect expressions for terminal velocity and time to reach the top of the trajectory. The correct terminal velocity is given by the formula vter = √(mg/c), and the user was advised to maintain consistent sign conventions throughout the calculations to avoid confusion.

PREREQUISITES
  • Understanding of classical mechanics principles, particularly projectile motion.
  • Familiarity with differential equations and their applications in physics.
  • Knowledge of drag forces, specifically quadratic drag in motion equations.
  • Proficiency in using LaTeX for mathematical expressions and notation.
NEXT STEPS
  • Review the derivation of equations of motion under quadratic drag.
  • Study the differences between hyperbolic and trigonometric functions, particularly arctanh and arctan.
  • Practice solving similar problems in vertical motion with varying drag coefficients.
  • Explore the implications of sign conventions in physics problems to enhance clarity in calculations.
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This discussion is beneficial for undergraduate students studying classical mechanics, physics educators, and anyone interested in mastering the concepts of projectile motion and drag forces in a physics context.

f3sicA_A
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Homework Statement
A projectile that is subject to quadratic air resistance is thrown vertically up with an initial speed ##v_0##. (a) Write down the equation of motion for the upwards motion and solve it to give ##v## as a function of ##t##. (b) Show that the time taken to reach the top of the trajectory is:

$$t_\mathrm{top}=(v_\mathrm{ter}/g)\tanh^{-1}{(v_0/v_\mathrm{ter})}$$
Relevant Equations
$$\pmb{f}=-cv^2\pmb{\hat{v}}$$
I am attempting problem number 2.38 from John R. Taylor's Classical Mechanics and I am not getting the correct answer. My procedure is as follows:

Equation of motion (taking up as the positive direction):

$$m\dot{v}=-mg-cv^2$$

Now to find ##v_\mathrm{ter}##, the terminal velocity, we consider the downward motion of the ball, that is, the velocity of the ball is in the downward direction, and therefore, we get:

$$-mg+cv^2=0$$

$$\implies v_\mathrm{ter}=\sqrt{\frac{mg}{c}}$$

I have a feeling I have made some sign convention error here but I am not sure what is wrong in my understanding. Continuing with this chain of reasoning:

$$\dot{v}=-g\left(1-\frac{v^2}{v_\mathrm{ter}}\right)$$

$$\implies \int_{v_0}^{v}\frac{1}{1-v'^2/v_\mathrm{ter}^2}\,\mathrm{d}v'=-g\int_0^t\,\mathrm{d}t'$$

$$\implies v_\mathrm{ter}\left[\tanh^{-1}{\frac{v'}{v_\mathrm{ter}}}\right]_{v_0}^v=-gt$$

$$\implies v_\mathrm{ter}\tanh^{-1}{\frac{v}{v_\mathrm{ter}}}=-gt+v_\mathrm{ter}\tanh^{-1}{\frac{v_0}{v_\mathrm{ter}}}$$

$$\implies v=v_\mathrm{ter}\tanh{\left[-\frac{gt}{v_\mathrm{ter}}+\tanh^{-1}{\left(\frac{v_0}{v_\mathrm{ter}}\right)}\right]}$$

From this, if I substitute ##v=0## to find ##t_\mathrm{top}##, I get:

$$t_\mathrm{top}=\left(\frac{v_\mathrm{ter}}{g}\right)\tanh^{-1}{\left(\frac{v_0}{v_\mathrm{ter}}\right)}$$

Whereas the answer requires that the function is arctan instead of hyperbolic arctan. Please let me know where I am going wrong, thank you!

Note: I am new to the forum and I am not very well-versed with the rules of this platform (I went through the basic guidelines) so in case I make some mistakes, please overlook them (and do let me know if I can do something to improve my presence on this platform). For context, I am an undergraduate student self-studying classical mechanics in the summer before my semester begins, thank you!
 
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You have ##v^2_{\text{ter}}=\dfrac{mg}{c}\implies c=\dfrac{mg}{ v^2_{\text{ter}} }.##

Replace that in the original equation. The relative sign between the two terms on the right hand side in the original equation is positive. Your algebra somehow changed it to negative. Redo the algebra more carefully this time.

It looks like this LaTeX does not recognize \arctanh (##\arctanh##) but it recognizes \tanh^{-1} (##\tanh^{-1}##).
 
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kuruman said:
The relative sign between the two terms on the right hand side in the original equation is positive. Your algebra somehow changed it to negative. Redo the algebra more carefully this time.
Thank you for your response! I am not sure which equations you are referring to, but I am guessing, I have made a mistake in the following equations:

$$m\dot{v}=-mg-cv^2$$

$$-mg+cv^2=0$$

I realize that I have changed the signs here; however, my logic behind this is that the in the first equation, the magnitude and direction ##-cv^2## is applied on the unit vector ##\pmb{\hat{v}}##; however, to take into account the changing direction of the unit vector itself, in the second equation where I write ##+cv^2##, it is as a magnitude of the unit vector ##\pmb{\hat{x}}##, and for doing this, I multiply the original magnitude ##-cv^2## by ##\cos{\theta}## where ##\theta## is the angle between ##\pmb{\hat{v}}## and ##\pmb{\hat{x}}##. Is this line of thinking faulty, or are you referring to some other equations?

Also, thank you for informing me about the LaTeX command for inverse hyperbolic tangent function, I have corrected that in the original question, along with the inline formulae.
 
Terminal velocity happens when ##\dot v=0##. Plug that into your first equation. Stop. Do not wave your hands. Why are you trying to wave your hands???
In 1 dimension a signed number is a vector
 
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f3sicA_A said:
I am not sure which equations you are referring to ##\dots##
##m\dot{v}=-mg-cv^2##

##v^2_{\text{ter}}=\dfrac{mg}{c}\implies c=\dfrac{mg}{ v^2_{\text{ter}} }.##

##m\dot{v}=-mg-\dfrac{mg}{ v^2_{\text{ter}} }v^2##

##\dot {v}=~?##
 
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hutchphd said:
In 1 dimension a signed number is a vector
Normally yes. In situations of this sort where you have damping that always opposes the velocity, I find that considerable confusion and grief are avoided if one follows the rule "choose as positive the direction of motion." Then the velocity and the speed are the same and one writes

##m\dfrac{dv}{dt}=-bv-mg~~## if the mass is moving up and both the damping force and the weight reduce the speed

##m\dfrac{dv}{dt}=-bv+mg~~## if the mass is moving down and the damping force reduces the speed while the weight increases it.

In either case symbol ##v## stands for speed not velocity which makes what's going on transparent.
 
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kuruman said:
##m\dot{v}=-mg-cv^2##

##v^2_{\text{ter}}=\dfrac{mg}{c}\implies c=\dfrac{mg}{ v^2_{\text{ter}} }.##

##m\dot{v}=-mg-\dfrac{mg}{ v^2_{\text{ter}} }v^2##

##\dot {v}=~?##
I realized where I made the mistake in signs, and now find it quite silly. I thank you for pointing that out.
 
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