Find time elapsed, given Force as a function f(velocity,displacment)

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The discussion revolves around calculating the time elapsed for a particle of mass 2 kg, initially moving at a velocity of π/2 m/s, under the influence of a resistance force defined as F = -2v tan(v) e^(2x). The user attempts to derive the relationship between displacement, velocity, and time using calculus, ultimately reaching a point where they struggle with the integral of a complex function. They receive suggestions to use a definite integral instead of an indefinite one to find the time taken for the particle to travel 1.55 m. The user later realizes their mistake and acknowledges the simplicity of the final step after taking a break.
Saracen Rue
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Homework Statement


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A particle of mass ## 2 kg ## is initially traveling with a constant velocity of ## \frac{\pi }{2}\ ms^{-1}##. The particle is acted upon by a resistance force, ## F=-2v\tan \left(v\right)e^{2x}##, where ##v## is the velocity in ##ms^{-1}## and ##x## is the displacement of the particle in meters at any time ##t##. Let ##t## be the time elapsed, in seconds, after the force is applied. Find the time taken for the particle to travel a distance of ##1.55 m##, expressing your answer in minutes correct to ##2## decimal places.

Homework Equations


Using calculus to convert between displacement, velocity and acceleration

##v=\frac{dx}{dt}##

##a=\frac{dv}{dt}=\frac{d^2x}{dt^2}=v\cdot \frac{dv}{dx}=\frac{d\left(\frac{1}{2}v^2\right)}{dx}##

The Attempt at a Solution


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##F=-2v\tan \left(v\right)e^{2x}##

##a=-v\tan \left(v\right)e^{2x}##

##v\cdot \frac{dv}{dx}=-v\tan \left(v\right)e^{2x}##

##\frac{v}{-v\tan \left(v\right)}dv=e^{2x}dx##

##\int _{ }^{ }-\cot \left(v\right)dv=\int _{ }^{ }e^{2x}dx##

##-\ln \left(\sin \left(v\right)\right)=\frac{1}{2}e^{2x}+c##

"initially traveling with a constant velocity of ##\frac{\pi }{2}\ ms^{-1}##"
Therefore at ##t=0##, ##v=\frac{\pi }{2}##. The question also states that ##x## is the displacement after the force has been applied, therefore at ##t=0##, ##x=0##.

##-\ln \left(\sin \left(v\right)\right)=\frac{1}{2}e^{2x}+c##

##-\ln \left(\sin \left(\frac{\pi }{2}\right)\right)=\frac{1}{2}e^{2\left(0\right)}+c##

##-\ln \left(1\right)=\frac{1}{2}+c##

Therefore, ##c=-\frac{1}{2}##

##-\ln \left(\sin \left(v\right)\right)=\frac{1}{2}e^{2x}-\frac{1}{2}##

##\sin \left(v\right)=e^{-\frac{1}{2}\left(e^{2x}-1\right)}##

##v=\arcsin \left(e^{-\frac{1}{2}\left(e^{2x}-1\right)}\right)##

##\frac{dx}{dt}=\arcsin \left(e^{-\frac{1}{2}\left(e^{2x}-1\right)}\right)##

##\frac{dt}{dx}=\frac{1}{\arcsin \left(e^{-\frac{1}{2}\left(e^{2x}-1\right)}\right)}##

##t=\int _{ }^{ }\frac{1}{\arcsin \left(e^{-\frac{1}{2}\left(e^{2x}-1\right)}\right)}dx##

This is where I get stuck. There's no way to get the integral of ##\frac{1}{\arcsin \left(e^{-\frac{1}{2}\left(e^{2x}-1\right)}\right)}## that I know of. I tried putting it into Wolfram Alpha but it said no result found in terms of standard mathematical functions. Have I done some of the intermediate steps wrong to arrive at this function which can't be integrated? Or is there another way of doing this? Any help is much appreciated.
 
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Your solution looks good to me...I would suggest using W|A to approximate the definite integral:

##\displaystyle t=\int_0^{1.55}\frac{1}{\arcsin\left(e^{-\frac{1}{2}\left(e^{2x}-1\right)}\right)}\,dx##
 
MarkFL said:
Your solution looks good to me...I would suggest using W|A to approximate the definite integral:

##\displaystyle t=\int_0^{1.55}\frac{1}{\arcsin\left(e^{-\frac{1}{2}\left(e^{2x}-1\right)}\right)}\,dx##

Sorry for late reply, I ended up realising to use a definite integral instead of an indefinite one on my own and forgot about this thread. I'm not sure what I was thinking trying to find the indefinite integral first - I guess I just needed a couple hour break before seeing how easy the final step actual was haha.

Anyway, thank you for your help regardless :)
 
Question: A clock's minute hand has length 4 and its hour hand has length 3. What is the distance between the tips at the moment when it is increasing most rapidly?(Putnam Exam Question) Answer: Making assumption that both the hands moves at constant angular velocities, the answer is ## \sqrt{7} .## But don't you think this assumption is somewhat doubtful and wrong?

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