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VICMath MethodsSyllabus dot point

How are related rates problems set up and solved using the chain rule and implicit differentiation?

The application of differentiation, including the chain rule, to related rates of change problems involving two or more time-dependent quantities

A focused answer to the VCE Math Methods Unit 4 key-knowledge point on related rates. The four-step procedure (relate variables, differentiate with respect to time, substitute, solve), the standard Paper 2 contexts (expanding circle, inflating sphere, sliding ladder, conical tank), and the common chain-rule traps.

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What this dot point is asking

VCAA wants you to handle word problems in which two or more time-dependent quantities are related by a geometric or algebraic equation, and one rate is known while another is asked for. The dot point pulls together the chain rule (Unit 3) and modelling reasoning. Paper 2 typically includes one related-rates problem per year.

The four-step procedure

Every related-rates problem yields to the same four steps.

Step 1. Identify the variables and relate them

Read the problem. Name the time-dependent variables (volume, radius, height, area, distance). Write the equation that relates them, drawn from geometry (cone, sphere, cylinder, triangle, circle), physics, or algebra.

If the equation has more variables than the question requires, eliminate the extras using auxiliary relationships (similar triangles, ratios, fixed proportions).

Step 2. Differentiate both sides with respect to time

Apply ddt\frac{d}{dt} to the entire equation. Each variable contributes its time derivative via the chain rule.

For example, if V=43Ο€r3V = \frac{4}{3} \pi r^3 and both VV and rr depend on time, then:

dVdt=43Ο€β‹…3r2β‹…drdt=4Ο€r2drdt\frac{dV}{dt} = \frac{4}{3} \pi \cdot 3 r^2 \cdot \frac{dr}{dt} = 4 \pi r^2 \frac{dr}{dt}

The factor drdt\frac{dr}{dt} comes from the chain rule because rr is a function of tt.

Step 3. Substitute the given numerical values

After differentiating, substitute the values at the specific moment the question describes. Note that the differentiation must happen before the substitution; you cannot plug in a value for rr first and then differentiate (because then VV would be a constant).

Step 4. Solve for the unknown rate

The equation from step 3 is linear in the unknown rate. Solve algebraically. State units.

Standard contexts

Expanding circle (area from radius)

Equation: A=Ο€r2A = \pi r^2.

Differentiate: dAdt=2Ο€rdrdt\frac{dA}{dt} = 2 \pi r \frac{dr}{dt}.

Use when a ripple or oil slick is expanding.

Inflating sphere (volume from radius, surface area from radius)

Volume: V=43Ο€r3V = \frac{4}{3} \pi r^3, so dVdt=4Ο€r2drdt\frac{dV}{dt} = 4 \pi r^2 \frac{dr}{dt}.

Surface area: S=4Ο€r2S = 4 \pi r^2, so dSdt=8Ο€rdrdt\frac{dS}{dt} = 8 \pi r \frac{dr}{dt}.

Use for balloons, bubbles.

Cylinder (volume from radius and height)

If both vary: V=Ο€r2hV = \pi r^2 h, dVdt=2Ο€rhdrdt+Ο€r2dhdt\frac{dV}{dt} = 2 \pi r h \frac{dr}{dt} + \pi r^2 \frac{dh}{dt} (product rule).

Often only one of rr or hh varies; the fixed variable drops.

Cone (similar-triangle reduction)

A conical tank with fixed total height HH and total radius RR. As water fills to depth hh with surface radius rr, the ratio rh=RH\frac{r}{h} = \frac{R}{H} holds. Eliminate rr to get V=Ο€R23H2h3V = \frac{\pi R^2}{3 H^2} h^3, a function of hh alone.

Use for water tanks, sand piles.

Sliding ladder

A ladder of length LL slides down a wall. Let xx be the horizontal distance from the wall to the foot of the ladder and yy the height of the top of the ladder.

Equation: x2+y2=L2x^2 + y^2 = L^2.

Differentiate: 2xdxdt+2ydydt=02 x \frac{dx}{dt} + 2 y \frac{dy}{dt} = 0, so dydt=βˆ’xydxdt\frac{dy}{dt} = -\frac{x}{y} \frac{dx}{dt}.

Use when an object slides along two perpendicular axes.

Trough or rectangular tank

A trough has cross-section of varying area as the water rises. Compute the cross-sectional area as a function of depth, then V=A(h)β‹…V = A(h) \cdot (length), giving dVdt=\frac{dV}{dt} = (length) β‹…Aβ€²(h)β‹…dhdt\cdot A'(h) \cdot \frac{dh}{dt}.

Worked example: receding shadow

A 1.8 m tall person walks away from a 5 m tall street lamp at 1.2 m/s. How fast is the tip of their shadow moving?

Step 1. Set up. Let xx be the distance from the lamp to the person and ss the distance from the lamp to the tip of the shadow. By similar triangles (lamp / shadow tip and person / shadow tip), 5s=1.8sβˆ’x\frac{5}{s} = \frac{1.8}{s - x}, giving 5(sβˆ’x)=1.8s5(s - x) = 1.8 s, i.e. 3.2s=5x3.2 s = 5 x, so s=2516xs = \frac{25}{16} x.

Step 2. Differentiate. dsdt=2516dxdt\frac{ds}{dt} = \frac{25}{16} \frac{dx}{dt}.

Step 3. Substitute. dxdt=1.2\frac{dx}{dt} = 1.2.

Step 4. Solve. dsdt=2516β‹…1.2=1.875\frac{ds}{dt} = \frac{25}{16} \cdot 1.2 = 1.875 m/s.

The tip of the shadow moves at 1.875 m/s, faster than the person.

Common errors

Substituting before differentiating. If you replace rr with 1010 before differentiating, you implicitly treat rr as constant, and drdt\frac{dr}{dt} disappears from the equation. Always differentiate first, then substitute.

Forgetting the chain rule. When differentiating r3r^3 with respect to tt (with rr a function of tt), the derivative is 3r2β‹…drdt3 r^2 \cdot \frac{dr}{dt}, not just 3r23 r^2.

Wrong sign on quantities that decrease. If the question says "water is draining at 5 L/min", dVdt=βˆ’5\frac{dV}{dt} = -5 (negative). If the question says "the ladder slides down", dydt\frac{dy}{dt} is negative.

Missing the elimination step. A cone problem with both rr and hh left in the volume formula gives an unsolvable equation. Use the similar-triangle relationship to reduce to a single variable before differentiating.

Units missing or wrong. Always include units. Watch for unit consistency (cm3^3/s vs L/min vs m3^3/min).

Not using the specific moment value. The question typically asks for the rate at a specific configuration (when r=10r = 10, when h=1h = 1). Substitute these values after differentiating.

In one sentence

A related-rates problem is solved by writing an equation that relates two or more time-dependent quantities (often from geometry or similar triangles), differentiating both sides with respect to time using the chain rule, substituting the given numerical values at the moment of interest, and solving the resulting linear equation for the unknown rate; the order of operations (differentiate first, substitute second) is the most heavily marked step.

Past exam questions, worked

Real questions from past VCAA papers on this dot point, with our answer explainer.

2024 VCAA Paper 24 marksA spherical balloon is being inflated such that its volume increases at a rate of $50$ cm$^3$ per second. Find the rate at which the radius is increasing when the radius is $10$ cm.
Show worked answer β†’

Step 1. Relate the variables. Volume of a sphere: V=43Ο€r3V = \frac{4}{3} \pi r^3.

Step 2. Differentiate both sides with respect to time tt.

dVdt=4Ο€r2β‹…drdt\frac{dV}{dt} = 4 \pi r^2 \cdot \frac{dr}{dt} (chain rule on r3r^3, where rr depends on tt).

Step 3. Substitute known values. dVdt=50\frac{dV}{dt} = 50 cm3^3/s; r=10r = 10 cm.

50=4Ο€(10)2β‹…drdt=400Ο€β‹…drdt50 = 4 \pi (10)^2 \cdot \frac{dr}{dt} = 400 \pi \cdot \frac{dr}{dt}.

Step 4. Solve.

drdt=50400Ο€=18Ο€\frac{dr}{dt} = \frac{50}{400 \pi} = \frac{1}{8 \pi} cm/s.

Approximately 0.03980.0398 cm/s.

Markers reward explicit relation between VV and rr, correct chain rule on r3r^3, substitution of the given rate and radius, and units in the final answer.

2023 VCAA Paper 25 marksWater is pouring into a conical tank with vertex at the bottom. The tank has height 4 m and radius 2 m at the top. Water flows in at a rate of $0.5$ m$^3$ per minute. Find the rate at which the water level is rising when the depth is 1 m.
Show worked answer β†’

Step 1. Relate the variables. Let hh be the depth of water and rr the radius of the water surface. By similar triangles, rh=24=12\frac{r}{h} = \frac{2}{4} = \frac{1}{2}, so r=h2r = \frac{h}{2}.

Volume of water: V=13Ο€r2h=13Ο€(h2)2h=Ο€h312V = \frac{1}{3} \pi r^2 h = \frac{1}{3} \pi \left( \frac{h}{2} \right)^2 h = \frac{\pi h^3}{12}.

Step 2. Differentiate with respect to time.

dVdt=Ο€12β‹…3h2β‹…dhdt=Ο€h24β‹…dhdt\frac{dV}{dt} = \frac{\pi}{12} \cdot 3 h^2 \cdot \frac{dh}{dt} = \frac{\pi h^2}{4} \cdot \frac{dh}{dt}.

Step 3. Substitute. dVdt=0.5\frac{dV}{dt} = 0.5 m3^3/min; h=1h = 1 m.

0.5=Ο€(1)24β‹…dhdt=Ο€4β‹…dhdt0.5 = \frac{\pi (1)^2}{4} \cdot \frac{dh}{dt} = \frac{\pi}{4} \cdot \frac{dh}{dt}.

Step 4. Solve.

dhdt=0.5Γ—4Ο€=2Ο€\frac{dh}{dt} = \frac{0.5 \times 4}{\pi} = \frac{2}{\pi} m/min.

Approximately 0.6370.637 m/min.

Markers reward the similar-triangle reduction (eliminating rr in favour of hh), the cubic-volume formula after substitution, correct chain rule, and units.

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