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Chapter 6 · Application of Derivatives

Example 30: Car with x=t2(2−t3)x=t^2\left(2-\frac{t}{3}\right)⁠: time to reach Q and distance PQ

ExamplesRate of change of quantities · Section 6.2 · Miscellaneous Examples
The question

A car starts from a point P at time t=0t = 0 seconds and stops at point Q. The distance xx⁠, in metres, covered by it, in tt seconds is given by

x=t2(2−t3)x = t^2\left(2 - \frac{t}{3}\right)

Find the time taken by it to reach Q and also find distance between P and Q.

Exam answer x=t2(2−t3)=2t2−t33x = t^2\left(2 - \frac{t}{3}\right) = 2t^2 - \frac{t^3}{3} v=dxdt=4t−t2=t(4−t)\begin{aligned} v = \frac{dx}{dt} &= 4t - t^2 \\ &= t(4 - t) \end{aligned}

v=0⇒t=0,4v = 0 \Rightarrow t = 0, 4⁠.

The car is at P at t=0t = 0⁠. For 0<t<40 < t < 4⁠, v>0v > 0⁠. So the car next stops, at Q, when t=4t = 4⁠.

At t=4t = 4⁠,

x=16(2−43)=323\begin{aligned} x &= 16\left(2 - \frac43\right) \\ &= \frac{32}{3} \end{aligned}

Hence the car reaches Q after 4 seconds, and the distance PQ is 323\dfrac{32}{3} m.

Want the reason behind every step, the basics and the checks?

The one idea this problem is built on

The rate of change of distance with respect to time is the velocity, v=dxdtv = \frac{dx}{dt}⁠. A car that stops has velocity zero. So we differentiate, find when v=0v = 0⁠, and pick the right instant: the car is also at rest at the very start (t=0t = 0⁠, at P), so Q is the next instant at which v=0v = 0⁠. Between the two instants the velocity must stay positive (the car keeps moving forward), and then the distance PQ is simply the value of xx at the stopping time.

Given, to find, and the plan
Given
Time tt in seconds from the start at P; distance covered xx in metres, with x=t2(2−t3)x = t^2\left(2 - \frac{t}{3}\right)⁠; the car stops at Q.
To find
The time taken to reach Q, and the distance PQ.
Plan
Expand xx⁠, differentiate to get vv⁠, solve v=0v = 0⁠. Check the sign of vv between the roots, so that the car really travels without stopping until the second root. Substitute that time into xx⁠.

Basics you need

1Velocity is a rate of change

Section 6.2 opens by recalling that dsdt\frac{ds}{dt} is the rate of change of distance ss with respect to time tt⁠. Here the distance is called xx⁠, so v=dxdtv = \frac{dx}{dt}⁠, measured in metres per second. Basics: rate of change as a derivative

2Power rule

ddt(tn)=n tn−1\frac{d}{dt}(t^n) = n\,t^{n-1}⁠, and a constant factor stays in front: ddt(c tn)=c n tn−1\frac{d}{dt}(c\,t^n) = c\,n\,t^{n-1} (Chapter 5).

3Sign of a product

A product of two factors is positive when both factors have the same sign and negative when their signs differ. It is zero exactly when one factor is zero. Basics: sign of a product

4A formula describes the situation only on its range

The formula for xx is a model of the car's journey from P to Q. Values of tt after the car has stopped are outside the situation, even though the formula still gives numbers there. Basics: building the function

Solution

  1. Expand the formula for the distance

    x=t2(2−t3)=2t2−t33.x = t^2\left(2 - \frac{t}{3}\right) = 2t^2 - \frac{t^3}{3}.
    A sum of powers of tt can be differentiated term by term with the power rule. Expanding first avoids the product rule (which would give the same answer with more work).
    Distributive law: t2⋅2=2t2t^2 \cdot 2 = 2t^2 and t2⋅t3=t33t^2 \cdot \frac{t}{3} = \frac{t^3}{3}⁠.
  2. Differentiate: the velocity

    v=dxdt=2⋅2t−3t23=4t−t2=t(4−t).v = \frac{dx}{dt} = 2 \cdot 2t - \frac{3t^2}{3} = 4t - t^2 = t(4 - t).

    The unit of vv is metres per second, because xx is in metres and tt in seconds.

    "Stops" is a statement about speed, not about position, so the question is really about vv⁠. Factorising 4t−t24t - t^2 by taking out the common factor tt makes it easy to see where vv is zero and what sign it has.
    Power rule: ddt(2t2)=4t\frac{d}{dt}(2t^2) = 4t and ddt(t33)=3t23=t2\frac{d}{dt}\left(\frac{t^3}{3}\right) = \frac{3t^2}{3} = t^2⁠. Basics: rate of change as a derivative
  3. When is the car at rest?

    v=0  ⟺  t(4−t)=0  ⟺  t=0  or  t=4.v = 0 \iff t(4 - t) = 0 \iff t = 0 \ \text{ or } \ t = 4.

    At t=0t = 0 the car is at P, just starting (it starts from rest). So t=0t = 0 is not the arrival at Q. The other root, t=4t = 4⁠, is the candidate for the stop at Q.

    A product is zero only when one of its factors is zero, so these are the only two instants with v=0v = 0⁠. The question tells us the car starts at P at t=0t = 0⁠; the zero velocity there is the moment of starting, not of stopping.
    Zero-product rule: ab=0ab = 0 exactly when a=0a = 0 or b=0b = 0⁠. Basics: factorising
  4. Check that the car keeps moving until t=4t = 4

    For 0<t<40 < t < 4⁠: the factor tt is positive and the factor 4−t4 - t is positive, so

    v=t(4−t)>0for 0<t<4.v = t(4 - t) > 0 \quad \text{for } 0 < t < 4.

    So after leaving P the car moves forward the whole time and does not stop before t=4t = 4⁠. The first stop after the start is at t=4t = 4⁠: the car reaches Q after 4 seconds.

    If vv became zero somewhere between 0 and 4, the car would have stopped there first, and that point would be Q. The sign check rules this out. It also shows that xx is increasing on [0,4][0, 4] (Theorem 1 of Section 6.3: xx is continuous and dxdt>0\frac{dx}{dt} > 0 inside the interval). In fact, because vv is strictly positive, the Mean Value Theorem step in the book's proof of Theorem 1 gives x(t2)>x(t1)x(t_2) > x(t_1) whenever t1<t2t_1 < t_2⁠: xx is strictly increasing, so the car never moves backwards.
    Sign of a product: both factors positive gives a positive product. Basics: sign of a product
  5. The distance from P to Q

    x∣t=4=42(2−43)=16⋅23=323 m.\begin{aligned} x\big|_{t=4} &= 4^2\left(2 - \frac{4}{3}\right) \\ &= 16 \cdot \frac{2}{3} = \frac{32}{3}\ \text{m}. \end{aligned}

    So PQ =323= \frac{32}{3} m =1023= 10\frac{2}{3} m, about 10.67 m.

    xx is the distance covered since leaving P. Because the car moved only forward (Step 4), the distance it covered is the same as the straight-line distance between P and Q.
    2−43=63−43=232 - \frac{4}{3} = \frac{6}{3} - \frac{4}{3} = \frac{2}{3}⁠.
  6. Why the formula is not used after t=4t = 4

    For t>4t > 4 the factor 4−t4 - t is negative, so the formula would give v<0v < 0⁠, and xx would fall back to 0 at t=6t = 6⁠. A negative "distance covered" rate is impossible for a car that has stopped at Q, so the formula only describes the journey for 0≤t≤40 \le t \le 4⁠.

    1 2 3 4 5 6 2 4 6 8 t (s) x (m) 32/3 P Q (t = 4, x = 32/3) flat tangent: v = 0 formula beyond t = 4: not used, car has stopped moving forward: v > 0
    xx against tt⁠. The solid curve is the journey: it rises from P and flattens at Q, where the tangent is horizontal (v=0v = 0⁠). The dashed part after t=4t = 4 is the formula, not the car.
    This answers a natural doubt: the formula is a model of one journey. Reading the graph, a student might be tempted to say the car "returns to P at t=6t = 6", but the question says the car stops at Q.
    A model is valid only on the range of the situation it describes. Basics: building the function
Result

The velocity is v=t(4−t)v = t(4 - t) m/s. It is zero at the start and next at t=4t = 4⁠, and positive in between. The car reaches Q after 4 seconds, and the distance PQ is 323\frac{32}{3} m (102310\frac{2}{3} m). (Textbook's own solution: 4 seconds and 323\frac{32}{3} m.)

Check it with numbers

Distances at whole seconds: x(1)=53≈1.6667x(1) = \frac{5}{3} \approx 1.6667⁠, x(2)=163≈5.3333x(2) = \frac{16}{3} \approx 5.3333⁠, x(3)=9x(3) = 9⁠, x(4)=323≈10.6667x(4) = \frac{32}{3} \approx 10.6667 m: they keep growing. Just before and after t=4t = 4⁠: x(3.9)=10.6470x(3.9) = 10.6470 and x(4.1)=10.6463x(4.1) = 10.6463⁠, both slightly less than 10.666710.6667⁠, as expected at the flat top. A difference quotient for the velocity at t=2t = 2⁠: x(2.001)−x(1.999)0.002≈4.0000\frac{x(2.001) - x(1.999)}{0.002} \approx 4.0000⁠, matching v(2)=2⋅2=4v(2) = 2 \cdot 2 = 4 m/s.

Common mistakes
  1. Solving x=0x = 0 instead of v=0v = 0⁠. x=0x = 0 at t=0t = 0 and t=6t = 6⁠, but x=0x = 0 means "no distance covered", which describes P, not Q. Stopping is about velocity.
  2. Answering t=0t = 0⁠. At t=0t = 0 the car is starting from rest at P. The arrival at Q is the next zero of vv⁠.
  3. Skipping the sign check. Without it we do not know that the car does not stop earlier, nor that distance covered equals PQ.
  4. Dropping the units. The time is 4 s and the distance is 323\frac{32}{3} m.
What to take away
  1. Velocity is dxdt\frac{dx}{dt}⁠; "starts" and "stops" are the instants where it is zero.
  2. Factorise the derivative: its zeros and its sign between them answer both "when" and "does it keep going".
  3. The fastest moment is in between: v=4t−t2v = 4t - t^2 is largest when dvdt=4−2t=0\frac{dv}{dt} = 4 - 2t = 0⁠, at t=2t = 2 s, with v=4v = 4 m/s.

Every fact used, and where it comes from

FactUsed inSource
Velocity =dxdt= \frac{dx}{dt}⁠, the rate of change of distanceSteps 2, 3Section 6.2, opening paragraph (Lesson: rate of change)
Power rule ddttn=ntn−1\frac{d}{dt}t^n = n t^{n-1}Step 2Chapter 5 (derivatives of polynomials)
Zero-product rule; sign of a productSteps 3, 4, 6Algebra
f′>0f' > 0 inside an interval and ff continuous gives ff increasingStep 4Theorem 1 and the Remarks after it, Section 6.3 (Lesson: increasing and decreasing)
Textbook working for this problemResultExample 30, Miscellaneous Examples, Chapter 6
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