We are given velocity as a function of time so integrating it with respect to time we will get he equation of displacement with respect to time
"v(t)=A(1-e^{-t\/t_{max}})"
"\\intop{dx}=\\intop A(1-e^{-t\/t_{max}})dt"
"x(t)=A" "t" "+A(e^{-t\/t{max}})t_{max}"
graph of the above function will be a linear one as e-t/tmax will be almost equal to zero
Differentiating velocity with respect to time we will get the acceleration
"a(t)=d" "(A(1-e^{-t\/t_{max}}))\/dt"
"a(t)=Ae^{-t\/t_{max}}\/t_{max}"
at t=0
acceleration= A/tmax
and as we tend towards infinity we see that the value of acceleration tends to become closer to zero hence the asymptote of this function is x-axis or a=0
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