A particle passes a fixed point OO and moves in a straight line such that, tt s after leaving OO, its velocity, v m/sv\text{ m/s}, is given by v=3t+2−t+23v = \frac{3}{t+2} - \frac{t+2}{3}. The particle reaches its greatest distance from OO at PP.

  1. (a)

    Find the time when the particle reaches PP.

  2. (b)

    Find the distance travelled by the particle when t=2t = 2.

  3. (c)

    Show that the velocity of the particle is decreasing at point PP.

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Worked solution

12(a)

1. Set velocity to zero to find the time when the particle reaches its greatest distance

At the greatest distance from OO, the particle is instantaneously at rest, so v=0v = 0.
3t+2−t+23=0\frac{3}{t+2} - \frac{t+2}{3} = 0

2. Solve the equation for $t$

3t+2=t+23\frac{3}{t+2} = \frac{t+2}{3}
(t+2)2=9(t+2)^2 = 9
t+2=3ort+2=−3t+2 = 3 \quad \text{or} \quad t+2 = -3
t=1ort=−5t = 1 \quad \text{or} \quad t = -5
Since t⩾0t \geqslant 0, t=1t = 1.

Answer

t=1t = 1

12(b)

1. Find the time when the particle changes direction (from part a).

The particle changes direction when v=0v = 0.
3t+2−t+23=0\frac{3}{t+2} - \frac{t+2}{3} = 0
(t+2)2=9(t+2)^2 = 9
t+2=3  ⟹  t=1t+2 = 3 \implies t = 1

2. Integrate velocity to find the displacement function $s(t)$.

s(t)=∫(3t+2−t+23)dts(t) = \int \left( \frac{3}{t+2} - \frac{t+2}{3} \right) dt
s(t)=3ln⁡(t+2)−(t+2)26+Cs(t) = 3 \ln(t+2) - \frac{(t+2)^2}{6} + C

3. Find the constant of integration $C$.

Since the particle passes OO at t=0t = 0, s(0)=0s(0) = 0.
0=3ln⁡(2)−226+C0 = 3 \ln(2) - \frac{2^2}{6} + C
C=23−3ln⁡2C = \frac{2}{3} - 3 \ln 2

4. Calculate the displacement at $t=1$ and $t=2$.

s(1)=3ln⁡(3)−326+23−3ln⁡2=3ln⁡(32)−56≈0.38306s(1) = 3 \ln(3) - \frac{3^2}{6} + \frac{2}{3} - 3 \ln 2 = 3 \ln\left(\frac{3}{2}\right) - \frac{5}{6} \approx 0.38306
s(2)=3ln⁡(4)−426+23−3ln⁡2=3ln⁡2−2≈0.07944s(2) = 3 \ln(4) - \frac{4^2}{6} + \frac{2}{3} - 3 \ln 2 = 3 \ln 2 - 2 \approx 0.07944

5. Calculate the total distance travelled.

Since the particle changes direction at t=1t=1, the total distance is the distance from t=0t=0 to t=1t=1 plus the distance from t=1t=1 to t=2t=2.
Distance=∣s(1)−s(0)∣+∣s(2)−s(1)∣\text{Distance} = |s(1) - s(0)| + |s(2) - s(1)|
Distance=s(1)+(s(1)−s(2))=2s(1)−s(2)\text{Distance} = s(1) + (s(1) - s(2)) = 2s(1) - s(2)
Distance=2(0.38306)−0.07944=0.68668≈0.687 m\text{Distance} = 2(0.38306) - 0.07944 = 0.68668 \approx 0.687\text{ m}

Answer

0.687 m0.687\text{ m}

12(c)

1. Differentiate the velocity function to find the acceleration $a$.

v=3(t+2)−1−13(t+2)v = 3(t+2)^{-1} - \frac{1}{3}(t+2)
a=dvdt=−3(t+2)−2−13a = \frac{dv}{dt} = -3(t+2)^{-2} - \frac{1}{3}
a=−3(t+2)2−13a = -\frac{3}{(t+2)^2} - \frac{1}{3}

2. Evaluate the acceleration at $t = 1$ (the time at point $P$ from part a) to show it is negative.

From part (a), at point PP, t=1t = 1.
Substitute t=1t = 1 into aa:
a=−3(1+2)2−13a = -\frac{3}{(1+2)^2} - \frac{1}{3}
a=−39−13=−23a = -\frac{3}{9} - \frac{1}{3} = -\frac{2}{3}
Since a<0a < 0, the velocity of the particle is decreasing at point PP.

Answer

Since a=−23<0a = -\frac{2}{3} < 0, the velocity is decreasing at PP.

AI analysis — may contain mistakes.

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