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Topos Uranos

Rates of change and related rates

Summary

This lesson reads the derivative as what it measures in applications: how fast one quantity changes when another changes. It distinguishes the average, the instantaneous and the relative rate of change, with their units, and characterizes growth at a constant relative rate. It studies motion along a line, with position, velocity, speed and acceleration, and proves what the sign of the derivative at an instant says, and what it does not say. Finally, when several quantities that depend on time are tied together by a relation, the chain rule also ties together their rates of change: these are related rates, which are solved with an explicit method.

Learning objectives

  1. Interpret the derivative as an instantaneous rate of change, with its units, and distinguish it from the average rate of change and from the relative one.
  2. Describe a rectilinear motion with position, velocity, speed and acceleration, and prove what the sign of the derivative at an instant says about nearby values.
  3. Solve related rates problems with an explicit method, justifying that the quantities being differentiated are differentiable.
  4. Relate the relative rates of change of products and powers to the logarithmic derivative, and accelerations to the second derivative of a relation.

The derivative as a rate of change

The lesson on the derivative as a limit arrived at the same definition from two questions: the slope of the tangent and the instantaneous velocity. Both are cases of a more general question. Whenever one quantity depends on another, the area of a circle on its radius, the position of a moving point on time, or the mass of a piece of rod on its length, it is worth knowing how fast the first changes when the second changes.

DefinitionRate of change

Let ff be a function defined on an open interval II, which expresses a quantity y=f(x)y = f(x) as a function of another quantity xx, and let aa and a+ha + h be points of II, with h≠0h \neq 0. The average rate of change of yy with respect to xx between aa and a+ha + h is the quotient

ΔyΔx=f(a+h)−f(a)h\frac{\Delta y}{\Delta x} = \frac{f(a + h) - f(a)}{h}

If ff is differentiable at aa, the instantaneous rate of change (or simply rate of change) of yy with respect to xx at aa is f′(a)f'(a); if moreover f(a)≠0f(a) \neq 0, the relative rate of change at aa is the quotient f′(a)f(a)\frac{f'(a)}{f(a)}.

The average rate is the slope of a secant, and the instantaneous rate, its limit: the slope of the tangent. Both are measured in units of yy per unit of xx: meters per second, if yy is a length and xx a time; kilograms per meter, if yy is the mass of a piece of rod and xx its length. In this last case, if M(x)M(x) is the mass of the piece between one end and the point at distance xx, the rate of change M′(x)M'(x) is the linear density of the rod at that point: the mass per unit length that a very short piece around it would have. The relative rate, by contrast, is measured only in reciprocal units of xx (per second, per day): it does not depend on the unit in which yy is measured, and for that reason it allows one to compare the change of quantities of different nature or of different size. It is the logarithmic derivative of the lesson on the variable in the exponent, and it is often expressed as a percentage: a relative rate of 0.030.03 per day is 3 percent per day.

A geometric example shows how a rate of change is read. The area of the circle of radius rr is A=πr2A = \pi r^2, and its rate of change with respect to the radius is dAdr=2πr\frac{\mathrm{d}A}{\mathrm{d}r} = 2\pi r, the circumference, as proposed problem 1 of the lesson on the derivative as a limit asks one to check. The reason is clear: when the radius increases by hh, the area increases by a ring of width hh, whose area is almost that of the circumference times hh.

PropositionGrowth at a constant relative rate

Let y0>0y_0 > 0 and k≠0k \neq 0 be real numbers, and let y(t)=y0ekty(t) = y_0 e^{kt} for every real tt. Then the relative rate of change of yy equals kk at every instant, and for every tt and every TT:

y(t+T)=ekT y(t)y(t + T) = e^{kT} \, y(t)

In particular, if k>0k > 0, the quantity doubles in every time interval of length ln⁡2k\frac{\ln 2}{k}, whatever the instant at which it begins; and if k<0k < 0, it is halved in every interval of length ln⁡2∣k∣\frac{\ln 2}{\abs{k}}.

Proof

  1. y′(t)=y0ekt⋅k=k y(t),y′(t)y(t)=ky'(t) = y_0 e^{kt} \cdot k = k \, y(t), \qquad \frac{y'(t)}{y(t)} = \resaltar{k}

    By the corollary on compositions with the exponential and the logarithm, from the lesson on the variable in the exponent, with u(t)=ktu(t) = kt, the function yy is differentiable on all of R\mathbb{R} and its derivative is kk times the function itself, which does not vanish.

  2. y(t+T)y(t)=y0ektekTy0ekt=ekT\frac{y(t + T)}{y(t)} = \frac{y_0 e^{kt} e^{kT}}{y_0 e^{kt}} = \resaltar{e^{kT}}

    By the law of exponents, the quotient between the values separated by an interval of length TT does not depend on tt.

  3. ekT=2⇔T=ln⁡2k,ekT=12⇔T=ln⁡2−ke^{kT} = 2 \Leftrightarrow T = \frac{\ln 2}{k}, \qquad e^{kT} = \frac{1}{2} \Leftrightarrow T = \resaltar{\frac{\ln 2}{-k}}

    Since the exponential is injective, the quotient equals 22 if and only if kT=ln⁡2kT = \ln 2, and equals 12\frac{1}{2} if and only if kT=−ln⁡2kT = -\ln 2.

A population of bacteria in an unrestricted medium or a mass of radioactive material changes, to a good approximation, at a constant relative rate, and the proposition explains why they have a fixed doubling time or half-life. That the functions y0ekty_0 e^{kt} are the only ones with constant relative rate kk is true, but its proof requires knowing that a function with zero derivative on an interval is constant, a consequence of the mean value theorem of the following unit.