MHB Solve Parameters of Displacement Function - Raja's Question

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The displacement function for a particle moving in a straight line is given by x(t) = e^(-3/4 t)(3 sin t + 4 cos t). The constants a and b are determined to be a = 3 and b = 4 based on initial conditions. The time taken for the particle to first reach the origin is approximately 2.21 seconds. Additionally, the particle attains its greatest negative displacement at around 3.14 seconds. The solution involves differentiating the displacement function to analyze velocity and using trigonometric identities for simplification.
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Here is the question:

How do you solve the following question?


A particle is moving in a straight line. The displacement x, from an origin O on the line, is given at time t by the equation x=e^(-3/4 t) (a sin t + b cos t).

Initially t=0, x=4, dx/dt = 0. Find the constants a and b. Determine also (i) the time elapsing from the start before the particle first reaches O, (ii) the time taken from O to attain the greatest displacement on the negative side of the origin.

I have posted a link there to this topic so the OP can see my work.
 
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Hello raja,

We are given the displacement function:

$$x(t)=e^{-\frac{3}{4}t}\left(a\sin(t)+b\cos(t) \right)$$

and we are told:

$$x(0)=4$$

And so this implies:

$$x(0)=e^{-\frac{3}{4}\cdot0}\left(a\sin(0)+b\cos(0) \right)=b=4$$

We may differentitate the displacement function with respect to time $t$ to obtain the velocity function:

$$v(t)=\frac{dx}{dt}=e^{-\frac{3}{4}t}\left(a\cos(t)-b\sin(t) \right)-\frac{3}{4}e^{-\frac{3}{4}t}\left(a\sin(t)+b\cos(t) \right)$$

We are given:

$$v(0)=0$$

Hence:

$$v(0)=e^{-\frac{3}{4}\cdot0}\left(a\cos(0)-b\sin(0) \right)-\frac{3}{4}e^{-\frac{3}{4}\cdot0}\left(a\sin(0)+b\cos(0) \right)=a-\frac{3}{4}b=a-3=0\,\therefore\,a=3$$

And so we have found:

$$a=3,\,b=4$$

Thus:

$$x(t)=e^{-\frac{3}{4}t}\left(3\sin(t)+4\cos(t) \right)$$

Using a linear combination identity, we may write this as:

$$x(t)=5e^{-\frac{3}{4}t}\sin\left(t+\tan^{-1}\left(\frac{4}{3} \right) \right)$$

i) Because the exponential factor has no real roots, to find the time it takes for the particle to first reach the origin, we simply need to equate the argument of the sine function to $\pi$:

$$t+\tan^{-1}\left(\frac{4}{3} \right)=\pi$$

$$t=\left(\pi-\tan^{-1}\left(\frac{4}{3} \right) \right)\text{ s}\approx2.21429743558818\text{ s}$$

ii) We may differentiate the displacement function to obtain the velocity function:

$$v(t)=5\left(e^{-\frac{3}{4}t}\cos\left(t+\tan^{-1}\left(\frac{4}{3} \right) \right)-\frac{3}{4}e^{-\frac{3}{4}t}\sin\left(t+\tan^{-1}\left(\frac{4}{3} \right) \right) \right)$$

$$v(t)=\frac{5}{4}e^{-\frac{3}{4}t}\left(4\cos\left(t+\tan^{-1}\left(\frac{4}{3} \right) \right)-3\sin\left(t+\tan^{-1}\left(\frac{4}{3} \right) \right) \right)$$

Using a linear combination identity, we may write:

$$v(t)=\frac{25}{4}e^{-\frac{3}{4}t}\sin\left(t+\tan^{-1}\left(\frac{4}{3} \right)+\tan^{-1}\left(-\frac{4}{3} \right)+\pi \right)$$

$$v(t)=-\frac{25}{4}e^{-\frac{3}{4}t}\sin(t)$$

Thus, we see by the first derivative test that the particle has a relative minimum at:

$$t=\pi\text{ s}\approx3.14159265358979\text{ s}$$

And because of the decaying amplitude, we know that for $0<t$, this is the global minimum.

Here is a plot of the displacement function:

View attachment 1431
 

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Here is a little puzzle from the book 100 Geometric Games by Pierre Berloquin. The side of a small square is one meter long and the side of a larger square one and a half meters long. One vertex of the large square is at the center of the small square. The side of the large square cuts two sides of the small square into one- third parts and two-thirds parts. What is the area where the squares overlap?

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