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@hartnn sambhalo plz
he will be able to help u better..:)
isnt velocity the derivative of position? v = s'
then the diffy q is can be written as s' = vo - ks s' + ks = vo and find solutions
your work looks fine, now recall that s(0) = 0, so when t=0, s=0
e^(a+b) = e^a e^b
since c is arbitrary then e^(kc) is arbitrary as well vo - ks = Ce^(kt)
now s' = vo - ks s' = Ce^(kt) calculate for s
s' = Ce^(-kt) ... :)
the thing is C is an arbitrary constant, its can be this or that or something else which makes e^kc an arbitrary constant in and of itself right?
what is the value of e^kc when c can be any value it wants to be?
why do u need to separate the constant ?
i dont see why s' = vo - ks = e^(kc-kt) = e^(kc) e^(-kt) s' = Ce^(-kt)
\(s = \dfrac{v_0 }{k}- Ce^{-kt} \) is the best you can simplify
@hartnn ok ..that's is what i wanted.. to simplify my answer
also for part b do we only differentiate v=v_0 -ks to get the eq for acceleration?
silly me, i was gonna work from s' into that :) solving for s outright seemed to simple lol
well, since s' = Ce^(-kt), acceleration is s''
v' would be easier :P
only after you plug in the function of s in terms of t in v
v' = -ks' ;) good luck
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