A particle PP moves in a straight line, so that, tt seconds after leaving a fixed point OO, its velocity, vv m/s, is given by v=10e−2t−3v = 10e^{-2t} - 3.

  1. (i)

    Find the initial velocity of PP.

  2. (ii)

    Find the acceleration of PP when t=1t = 1.

  3. (iii)

    Find the value of tt when PP is at instantaneous rest.

  4. (iv)

    Find the total distance travelled by PP before it comes to instantaneous rest.

  5. (v)

    Explain why the value of vv is always greater than −3-3.

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Worked solution

11(i)

1. Substitute $t = 0$ into the velocity equation to find the initial velocity

When t=0t = 0,
v=10e−2(0)−3v = 10e^{-2(0)} - 3
v=10(1)−3v = 10(1) - 3
v=7v = 7

Answer

7 m/s7\text{ m/s}

11(ii)

1. Find the expression for acceleration by differentiating velocity with respect to time

a=dvdt=ddt(10e−2t−3)=−20e−2ta = \frac{dv}{dt} = \frac{d}{dt}(10e^{-2t} - 3) = -20e^{-2t}

2. Substitute $t = 1$ to find the acceleration

When t=1t = 1,
a=−20e−2(1)=−20e−2≈−2.71 m/s2a = -20e^{-2(1)} = -20e^{-2} \approx -2.71 \text{ m/s}^2

Answer

−20e−2-20e^{-2} m/s2^2 (or −2.71-2.71 m/s2^2)

11(iii)

1. Set velocity to zero for instantaneous rest

For instantaneous rest, v=0v = 0.
10e−2t−3=010e^{-2t} - 3 = 0

2. Isolate the exponential term

10e−2t=310e^{-2t} = 3
e−2t=0.3e^{-2t} = 0.3

3. Solve for $t$ using natural logarithms

−2t=ln⁡0.3-2t = \ln 0.3
t=−12ln⁡0.3t = -\frac{1}{2} \ln 0.3
t≈0.601986t \approx 0.601986
t≈0.602 (to 3 s.f.)t \approx 0.602 \text{ (to 3 s.f.)}

Answer

t=0.602t = 0.602

11(iv)

1. Find the time $t$ when the particle is at instantaneous rest (from part iii).

At instantaneous rest, v=0v = 0.
10e−2t−3=010e^{-2t} - 3 = 0
e−2t=0.3e^{-2t} = 0.3
−2t=ln⁡0.3-2t = \ln 0.3
t=−12ln⁡0.3≈0.601986t = -\frac{1}{2}\ln 0.3 \approx 0.601986

2. Set up the definite integral for the distance travelled.

Since v>0v > 0 for 0⩽t<0.6019860 \leqslant t < 0.601986, the distance travelled is the integral of vv from t=0t = 0 to t=0.601986t = 0.601986.
Distance=∫00.601986(10e−2t−3) dt\text{Distance} = \int_0^{0.601986} (10e^{-2t} - 3) \, dt

3. Integrate the velocity function.

∫(10e−2t−3) dt=[10e−2t−2−3t]00.601986\int (10e^{-2t} - 3) \, dt = \left[ \frac{10e^{-2t}}{-2} - 3t \right]_0^{0.601986}
=[−5e−2t−3t]00.601986= \left[ -5e^{-2t} - 3t \right]_0^{0.601986}

4. Evaluate the definite integral to find the final distance.

=(−5e−2(0.601986)−3(0.601986))−(−5e0−0)= \left( -5e^{-2(0.601986)} - 3(0.601986) \right) - \left( -5e^0 - 0 \right)
=(−5(0.3)−1.805958)−(−5)= \left( -5(0.3) - 1.805958 \right) - (-5)
=−1.5−1.805958+5= -1.5 - 1.805958 + 5
=1.69404≈1.69 m (to 3 s.f.)= 1.69404 \approx 1.69 \text{ m (to 3 s.f.)}

Answer

1.691.69 m

11(v)

1. State the property of the exponential function

For all real values of tt, e−2t>0e^{-2t} > 0.

2. Deduce the inequality for $v$

Since e−2t>0e^{-2t} > 0, it follows that 10e−2t>010e^{-2t} > 0.
Therefore, v=10e−2t−3>0−3=−3v = 10e^{-2t} - 3 > 0 - 3 = -3.

Answer

Since e−2t>0e^{-2t} > 0 for all tt, 10e−2t>010e^{-2t} > 0, which means v=10e−2t−3>−3v = 10e^{-2t} - 3 > -3.

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