Solved Problem on Kinematics
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Two bodies are in a straight line with constant acceleration on the same trajectory, their motions are described by the equations
\[ \begin{gather} \left. \begin{array}{l} x_{1}=2t-\dfrac{1}{2}t^{2}\\[5pt] x_{2}=10-3t+\dfrac{3}{2}t^{2} \end{array} \right. \qquad\text{(}\mathit{S.I.}\text{ units)} \end{gather} \]
Determine:
a) The position where they meet;
b) The instant of time that the distance between the two bodies is the smallest and the distance between them;
c) The instant of time in which the speeds of the bodies change direction and their positions.


Solution

a) When bodies meet their positions should be equal
\[ \begin{gather} x_{1}=x_{2}\\ 2t-\frac{1}{2}t^{2}=10-3t+\frac{3}{2}t^{2}\\ 10-3t+\frac{3}{2}t^{2}-2t+\frac{1}{2}t^{2}=0\\ 10-5t+2t^{2}=0\\[10pt] \Delta=(-5)^{2}-4\times 2\times 10\\ \Delta =25-80\\ \Delta =-55 \end{gather} \]
As Δ < 0 this means that no x satisfies the two equations at the same time, the bodies do not meet.

b) At any point, the distance between bodies is given by the difference in their positions
\[ \begin{gather} x=x_{2}-x_{1}\\ x=10-3t+\frac{3}{2}t^{2}-\left(2t-\frac{1}{2}t^{2}\right)\\ x=10-3t+\frac{3}{2}t^{2}-2t+\frac{1}{2}t^{2}\\ x=10-5t+2t^{2} \tag{I} \end{gather} \]
To determine the minimum distance, we take the derivative of this function with respect to time, and equal to zero
\[ \begin{gather} \frac{dx}{dt}=-5+4t=0 \tag{II}\\ 4t=5 \end{gather} \]
\[ \bbox[#FFCCCC,10px] {t=\frac{5}{4}=1.25\;\text{s}} \]
To verify if this is the minimum point of the function, we take the second derivative, deriving the expression (II)
\[ \frac{d^{2}x}{dt^{2}}=4 > 0 \]
as the second derivative is greater than zero the instant found represents a minimum point of the function.
Substituting the instant of time calculated in the expression (I), we find the minimum xmin distance between the bodies
\[ \begin{gather} x_{min}=10-5\times \frac{5}{4}+2\times \left(\frac{5}{4}\right)^{2}\\ x_{min}=10-\frac{25}{4}+2\times \frac{25}{16}\\ x_{min}=10-\frac{25}{4}+\frac{50}{16}\\ x_{min}=\frac{160-100+50}{16}\\ x_{min}=\frac{110}{16} \end{gather} \]
\[ \bbox[#FFCCCC,10px] {x_{min}=6.875\;\text{m}} \]

c) To find the expressions of velocities as a function of time for bodies of 1 and 2, we take the derivative of their expressions with respect to time, for the body 1
\[ \frac{dx_{1}}{dt}=v_{1}=2-t \]
when the speed changes direction it equals zero, v1 = 0
\[ 0=2-t \]
\[ \bbox[#FFCCCC,10px] {t=2\;\text{s}} \]
substituting this value in the expression for x1, the position will be
\[ \begin{gather} x_{1}=2\times 2-\frac{1}{2}\times 2^{2}\\ x_{1}=4-\frac{4}{2}\\ x_{1}=4-2 \end{gather} \]
\[ \bbox[#FFCCCC,10px] {x_{1}=2\;\text{m}} \]
For body 2
\[ \frac{dx_{2}}{dt}=v_{2}=-3+3t \]
when the speed changes direction it equals zero, v2 = 0
\[ \begin{gather} 0=-3+3t\\ 3t=3\\ t=\frac{3}{3} \end{gather} \]
\[ \bbox[#FFCCCC,10px] {t=1\;\text{s}} \]
substituting this value in the expression for x2, the position will be
\[ \begin{gather} x_{2}=10-3.1+\frac{3}{2}\times 1^{2}\\ x_{2}=10-3+\frac{3}{2}\\ x_{2}=\frac{20-6+3}{2}\\ x_{2}=\frac{17}{2} \end{gather} \]
\[ \bbox[#FFCCCC,10px] {x_{2}=8.5\;\text{m}} \]
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