Question #95073
(a) You and your new alien friend, Howard need to escape area 51 fast! Luckily, Howard knows of a high-end sports car you can use in your escape. Assuming you don't get shot in the process, what is the minimum acceleration necessary to reach a linear displacement of 5.00 km in under 2.00 minutes? Assume you start from rest and maintain a constant acceleration. (b) Howard's Bugatti has a maximum acceleration around 11.0 m/s2 and a top speed of about 260.0 mph. What is the least amount of time it will take you to reach a linear displacement of 5.00 km if you accelerate at a constant rate of 11.0 m/s until reaching top speed and then cruise at the top speed for the remainder of the trip into Mexico? (
1
Expert's answer
2019-09-23T09:34:01-0400

a)Using the law for uniformly accelerated motion we can express a travelled distance in time tt (and we use the condition that we start from the rest v0=0{v_0} = 0)


l=v0t+at22=at22l = {v_0}t + \frac{{a{t^2}}}{2} = \frac{{a{t^2}}}{2}


Expressing acceleration


a=2lt2a = 2\frac{l}{{{t^2}}}


We get minimal value of acceleration needed to reach the given displacement if we give a travelled distance is equal to the given displacement. Now do the calculations


amin=2lt2=25[km]22[min2]=25103[m]22602[s2]=2536[ms2]0.7[ms2]{a_{\min }} = 2\frac{l}{{{t^2}}} = 2\frac{{5[{\text{km}}]}}{{{2^2}[{{\min }^2}]}} = 2\frac{{5 \cdot {{10}^3}[{\text{m}}]}}{{{2^2} \cdot {{60}^2}[{{\text{s}}^2}]}} = \frac{{25}}{{36}}[\frac{{\text{m}}}{{{{\text{s}}^2}}}] \approx 0.7[\frac{{\text{m}}}{{{{\text{s}}^2}}}]

b)At the first let's evaluate the time needed to reach the top speed from the rest (denote it by τ\tau) . Use the law for uniformly accelerated motion


v=v0+aτ=aτv = {v_0} + a\tau = a\tauτ=va\tau= \frac{v}{a}

We will need to convert mph in m/s, it's can be done by multiplying by 0.447{0.447}. Thus


τ=vmaxa=260[mph]11[ms2]0.447260[ms]11[ms2]10.566[s]\tau = \frac{{{v_{\max }}}}{a} = \frac{{260[{\text{mph]}}}}{{11[\frac{{\text{m}}}{{{{\text{s}}^{\text{2}}}}}]}} \approx \frac{{0.447 \cdot 260[\frac{{\text{m}}}{{\text{s}}}{\text{]}}}}{{11[\frac{{\text{m}}}{{{{\text{s}}^{\text{2}}}}}]}} \approx 10.566[{\text{s}}]

In this time the car travelled


d=at22=1211[ms2]10.5662[s2]=614.022[m]d = \frac{{a{t^2}}}{2} = \frac{1}{2} \cdot 11[\frac{{\text{m}}}{{{{\text{s}}^{\text{2}}}}}] \cdot {10.566^2}[{{\text{s}}^2}] = 614.022[{\text{m}}]

The rest part of the full distance x=ldx = l - d the car will move with constant (top) speed. It will take the time


t=ldvmax=5[km]614.022[m]260[mph]5103[m]614.022[m]0.447260[ms]37.739[s]t = \frac{{l - d}}{{{v_{\max }}}} = \frac{{5[{\text{km}}] - 614.022[{\text{m}}]}}{{260[{\text{mph]}}}} \approx \frac{{5 \cdot {{10}^3}[{\text{m}}] - 614.022[{\text{m}}]}}{{0.447 \cdot 260[\frac{{\text{m}}}{{\text{s}}}{\text{]}}}} \approx 37.739[{\text{s}}]

Thus the full time to reach the given displacement is


tfull=t+τ=10.566[s]+37.739[s]=48.305[s]48.3[s]{t_{{\text{full}}}} = t + \tau = 10.566[{\text{s}}] + 37.739[{\text{s}}] = 48.305[{\text{s}}] \approx 48.3[{\text{s}}]

This is the answer to part b)



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