Not your typical car problem

Calculus Level 5

A certain road follows the path of a sine wave, with the equation y = sin ( π 6 x ) y = \sin \left(\frac {\pi}{6} x\right) , whose origin represents the starting point of the road. If a car is travelling at this road starting at its origin, at an instantaneous speed of 9 x 2 3 x 2 1 1 + π 2 36 cos 2 ( π 6 x ) \frac { 9x^2}{3x^2 - 1} \sqrt{1+ \frac {\pi^2}{36}\cos^{2}\left( \frac{\pi}{6}x\right)} m/s, as the car moves farther, determine the limiting rate (in m/s) as to how the car separates from the origin.

Note:

The values of x x and y y are in meters.

Clarification: In the graph above, the car follows the red path.


The answer is 3.

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1 solution

Efren Medallo
Jun 19, 2015

The instantaneous distance of the car from the origin (shown in violet), can be represented by y = ( x 2 + s i n 2 ( π 6 x ) ) y = \sqrt ( x^2 + sin^2 (\frac{\pi}{6}x)) .

By virtue of related rates, we see that

d y d t = d y d x d x d t \large \frac{dy}{dt}=\frac{dy}{dx}\cdot \frac{dx}{dt}

However, instead of d x d t \frac{dx}{dt} , we are given with the rate of the car along the graph of y = s i n ( π 6 x ) y = sin(\frac{\pi}{6} x) . If we let this given rate as d L d t \frac{dL}{dt} , then we can derive a relationship that

d x d t = d x d L d L d t \large \frac{dx}{dt}=\frac{dx}{dL}\cdot \frac{dL}{dt} , simplifying our original equation to

d y d t = d y d x d x d L d L d t \large \frac{dy}{dt}=\frac{dy}{dx}\cdot \frac{dx}{dL}\cdot \frac{dL}{dt}

Now, we will have to find d x d L \frac{dx}{dL} . Note that L = 1 + ( y ) 2 d x L =\large \int \:\sqrt{1+\left(y'\right)^2}dx

thus, d L d x = 1 + π 2 36 c o s ( π 6 x ) \large \frac {dL}{dx} = \sqrt {1+ \frac{\pi^2}{36}cos(\frac{\pi}{6}x)} .

It follows that

d x d L = 1 1 + π 2 36 c o s ( π 6 x ) \large \frac {dx}{dL} = \frac{1}{\sqrt {1+ \frac{\pi^2}{36}cos(\frac{\pi}{6}x)}} .

Now, we have d x d L \large \frac {dx}{dL} and d L d t \frac {dL}{dt} . We can easily get the derivative d y d x \frac {dy}{dx} and get

6 x + π sin ( π x 6 ) cos ( π x 6 ) 6 x 2 + sin 2 ( π x 6 ) \large\frac{6x+\pi \sin \left(\frac{\pi x}{6}\right)\cos \left(\frac{\pi x}{6}\right)}{6\sqrt{x^2+\sin ^2\left(\frac{\pi x}{6}\right)}} .

So,

d y d t = d y d x d x d L d L d t \large \frac {dy}{dt} = \frac {dy}{dx} \cdot \frac {dx}{dL} \cdot \frac {dL}{dt} and get 6 x + π sin ( π x 6 ) cos ( π x 6 ) 6 x 2 + sin 2 ( π x 6 ) 1 1 + p i 2 36 c o s ( p i 6 x ) 9 x 2 3 x 2 1 1 + π 2 36 c o s 2 π 6 x \frac{6x+\pi \sin \left(\frac{\pi x}{6}\right)\cos \left(\frac{\pi x}{6}\right)}{6\sqrt{x^2+\sin ^2\left(\frac{\pi x}{6}\right)}} \cdot \frac{1}{\sqrt {1+ \frac{pi^2}{36}cos(\frac{pi}{6}x)} }\cdot \frac { 9x^2}{3x^2 - 1} \sqrt{1+ \frac {\pi^2}{36}cos^{2} \frac{\pi}{6}x}

Simplifying that, we get

d y d x = 6 x + π sin ( π x 6 ) cos ( π x 6 ) 6 x 2 + sin 2 ( π x 6 ) 9 x 2 3 x 2 1 \frac {dy}{dx} = \large \frac{6x+\pi \:\sin \:\left(\frac{\pi \:x}{6}\right)\cos \:\left(\frac{\pi \:x}{6}\right)}{6\sqrt{x^2+\sin \:^2\left(\frac{\pi \:x}{6}\right)}}\cdot \frac{9x^2}{3x^2-1} .

We are asked to find out lim x ( d y d x ) \lim _{x\to \infty }\left(\frac{dy}{dx}\right) .

And here, by use of squeeze theorem, L'Hopital's rule and other related theorems,

lim x ( 6 x + π sin ( π x 6 ) cos ( π x 6 ) 6 x 2 + sin 2 ( π x 6 ) 9 x 2 3 x 2 1 ) = 3 \large \lim _{x\to \infty }\left(\frac{6x+\pi \sin \:\:\left(\frac{\pi \:\:x}{6}\right)\cos \left(\frac{\pi \:\:x}{6}\right)}{6\sqrt{x^2+\sin ^2\left(\frac{\pi \:\:x}{6}\right)}}\cdot \frac{9x^2}{3x^2-1}\:\right) = \boxed {3}

This question doesn't make sense. For the small x, the speed is negative. Speed can't be negative.

Joe Mansley - 3 months, 4 weeks ago

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