Rates of change

Drop a stone in a pond and the ripple's radius grows every second — but how fast is the enclosed area growing at the exact instant the ripple is six metres across? That question cannot be answered by comparing two positions; it needs the derivative, the tool built precisely to measure change at an instant rather than over an interval. This is the derivative doing real work: converting a word problem about an expanding oil spill, a sliding ladder, or a draining tank into a clean equation you can solve. The technique is called related rates — two quantities are tied together by a fixed geometric or physical relationship, and differentiating that relationship with respect to time links their two rates of change, even when neither quantity's explicit formula in terms of time is ever known.

The core insight

Whenever two changing quantities are connected by a fixed equation, differentiating that equation with respect to time — using the chain rule on every time-varying quantity — relates their instantaneous rates of change.

The core idea

If a quantity yy depends on time tt, either directly or through another variable xx, then dydt\dfrac{dy}{dt} is its instantaneous rate of change — positive if yy is increasing, negative if it is decreasing. Most physical situations do not hand you yy as an explicit function of tt; instead they hand you a relationship between two changing quantities, such as a geometric formula, and tell you how fast one of them is changing. The bridge between the two is the chain rule. If y=f(x)y = f(x) and both xx and yy vary with tt, then

dydt=f′(x)⋅dxdt\frac{dy}{dt} = f'(x)\cdot\frac{dx}{dt}

where: xx and yy are the two related quantities, ff is the function connecting them (so y=f(x)y=f(x) at every instant), and dxdt\dfrac{dx}{dt}, dydt\dfrac{dy}{dt} are their respective rates of change with time. Every related-rates problem follows the same three moves: identify the relating equation between the quantities involved (an area, volume, or Pythagoras-type formula), differentiate that equation with respect to tt — attaching a chain-rule rate factor to every time-varying quantity, not just one — and only then substitute the known numerical values to solve for the unknown rate. Two things make this technique so useful in practice. First, you almost never need to know x(t)x(t) or y(t)y(t) explicitly — real problems only ever hand you a snapshot rate and a snapshot value, not full functions of time, and related rates works with exactly that limited information. Second, the technique reduces every new scenario to the same short checklist: name the changing quantities, write the geometric or physical law that ties them together, differentiate once with respect to tt, and substitute. Once that pattern is internalised, circles, spheres, cones and right-triangle setups all become the same three lines of algebra with a different relating equation plugged in.

Figure
A circle whose radius and area both grow with time, showing the rate of change of the radius feeding through the chain rule into the rate of change of the area
A growing circle links dr/dt to dA/dt r dr/dt radius r grows steadily outward A = pi r^2 dA/dt = 2 pi r . dr/dt differentiate the relating equation with respect to t, chain rule on r

The goal is to derive the general working rule used in every related-rates problem: given any relating equation linking two quantities such as y=f(x)y=f(x), produce the equation that links their rates dxdt\dfrac{dx}{dt} and dydt\dfrac{dy}{dt}, so that a single differentiation step turns a static geometric formula into a dynamic one usable for word problems where only rates and one instant are known, never the full functions of time.

Step 1. Start from the relating equation. Suppose two quantities are connected by y=f(x)y = f(x) — this could be A=πr2A = \pi r^2 for a circle's area and radius, or V=43πr3V = \tfrac{4}{3}\pi r^3 for a sphere's volume and radius, or any similar geometric or physical formula. Both xx and yy are understood to be functions of time tt, even though neither is written out explicitly.

Step 2. Differentiate both sides with respect to tt. Because yy is a function of xx, and xx is itself a function of tt, the left side needs the chain rule: ddt[f(x)]=f′(x)⋅dxdt\dfrac{d}{dt}\big[f(x)\big] = f'(x)\cdot\dfrac{dx}{dt}. So differentiating y=f(x)y=f(x) throughout with respect to tt gives dydt=f′(x)⋅dxdt\dfrac{dy}{dt} = f'(x)\cdot\dfrac{dx}{dt}.

Step 3. Read off the working rule. Every term that involves a changing quantity picks up a rate factor for that quantity; nothing is ever differentiated with respect to xx alone. This is why the method is called related rates: the equation now expresses one rate directly in terms of the other rate and the instantaneous value of xx, which is exactly the form needed to substitute numbers and solve for whichever rate is unknown.

Step 4. Confirm with the circle. For A=πr2A=\pi r^2, f(r)=πr2f(r)=\pi r^2 so f′(r)=2πrf'(r)=2\pi r, giving dAdt=2πr⋅drdt\dfrac{dA}{dt} = 2\pi r\cdot\dfrac{dr}{dt} — precisely the formula used below, and the pattern every related-rates setup in this syllabus (circles, spheres, cones, right triangles) follows.

Worked example

The radius of a circular oil spill is increasing at a rate of 0.50.5 m/s. Find the rate at which the area of the spill is increasing when the radius is 66 m.

Step 1. Write the relating equation: A=πr2A = \pi r^2.

Step 2. Differentiate with respect to tt, applying the chain rule since r=r(t)r=r(t): dAdt=2πr⋅drdt\dfrac{dA}{dt} = 2\pi r\cdot\dfrac{dr}{dt}.

Step 3. Substitute the known values, drdt=0.5\dfrac{dr}{dt}=0.5 m/s and r=6r=6 m: dAdt=2π(6)(0.5)=6π\dfrac{dA}{dt} = 2\pi(6)(0.5) = 6\pi.

Step 4. State the result with units: dAdt=6π≈18.85 m2/s\dfrac{dA}{dt} = 6\pi \approx 18.85\ \text{m}^2/\text{s}.

The area of the oil spill is increasing at 6π m2/s≈18.85 m2/s6\pi\ \text{m}^2/\text{s} \approx 18.85\ \text{m}^2/\text{s} when r=6r=6 m.

Competitive stretch

A 55 m ladder leans against a wall; its foot is pulled away from the wall at 0.30.3 m/s. Let xx be the foot's distance from the wall and yy the height of the top on the wall, so x2+y2=25x^2+y^2=25. Differentiating gives 2xdxdt+2ydydt=02x\dfrac{dx}{dt}+2y\dfrac{dy}{dt}=0. At x=3x=3, Pythagoras gives y=4y=4. Substituting dxdt=0.3\dfrac{dx}{dt}=0.3: 2(3)(0.3)+2(4)dydt=0⇒dydt=−1.88=−0.2252(3)(0.3)+2(4)\dfrac{dy}{dt}=0 \Rightarrow \dfrac{dy}{dt} = \dfrac{-1.8}{8} = -0.225. The top slides down at 0.2250.225 m/s — the negative sign confirming yy is decreasing — when the foot is 33 m from the wall. Both examples above share the same shape: one geometric fact fixed for all time (the circle's area formula, or the ladder's constant length via Pythagoras), one given rate, and one instant at which the unknown rate is wanted. Recognising that shape — rather than memorising each scenario separately — is what lets the same three-step method handle spheres filling with water, cones draining, shadows lengthening, and any other pair of quantities tied together by a fixed relationship.

Common traps

  • Differentiating the relating equation with respect to xx instead of tt — every time-varying quantity needs a chain-rule rate factor like dxdt\dfrac{dx}{dt}, not a bare derivative.
  • Substituting numerical values before differentiating — this destroys the variable you still need to differentiate against; always differentiate the general relation first, then plug in numbers.
  • Dropping or misreading the sign of a rate — a decreasing quantity must appear as a negative rate, as in the sliding-ladder example.
  • Forgetting to find an intermediate value (like yy from Pythagoras) needed to evaluate the final rate at the specific instant asked about.

Ask the tutor: Got a cone-shaped tank draining or a similar related-rates setup you are stuck on — bring your relating equation to the AI tutor and work through the differentiation together.

Why do we differentiate with respect to t instead of just solving for the rate directly?

Because the relating equation, like A=πr2A=\pi r^2, holds at every instant but does not by itself tell you how fast anything changes — it is a snapshot, not a rate. Differentiating it with respect to time converts the static geometric relationship into a dynamic one linking the two rates, dAdt\dfrac{dA}{dt} and drdt\dfrac{dr}{dt}. Only after this step do the given rate and the value at the instant in question let you solve algebraically for the unknown rate.

How do I know which quantities need a chain-rule rate term and which do not?

Any quantity that changes with time in the scenario needs a rate term the moment you differentiate it — this includes every variable in the relating equation, such as rr in A=πr2A=\pi r^2 or both xx and yy in x2+y2=25x^2+y^2=25. Constants, like the fixed length of the ladder, never get a rate term because they do not change. A quick check: if the problem gives or asks for "the rate at which ___ changes," that quantity needs d(⋅)/dtd(\cdot)/dt attached wherever it appears.

Can related rates be negative, and what does that mean physically?

Yes, and the sign carries real meaning: a positive rate means the quantity is increasing with time, a negative rate means it is decreasing. In the ladder example, dydt=−0.225\dfrac{dy}{dt}=-0.225 m/s tells you the height on the wall is falling, even though the given rate for the foot's motion, dxdt=0.3\dfrac{dx}{dt}=0.3 m/s, was positive. Always interpret the sign in context rather than reporting only the magnitude.

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