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

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SUMMARY

The discussion focuses on calculating the time elapsed for a particle of mass 2 kg, initially traveling at a velocity of π/2 m/s, under the influence of a resistance force defined by F = -2v tan(v) e^(2x). The user successfully derives the relationship between displacement, velocity, and acceleration using calculus, ultimately expressing the time taken to travel 1.55 m as a definite integral. The integral t = ∫(1/arcsin(e^(-1/2(e^(2x)-1)))) dx from 0 to 1.55 is recommended for approximation using Wolfram Alpha.

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Saracen Rue
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Homework Statement


[/B]
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


[/B]
##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 :)
 

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