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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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  1. What this dot point is asking
  2. The four-step procedure
  3. Standard contexts
  4. Worked example: receding shadow
  5. Examples in context
  6. Try this

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=43πr3V = \frac{4}{3} \pi r^3 and both VV and rr depend on time, then:

dVdt=43π3r2drdt=4πr2drdt\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=πr2A = \pi r^2.

Differentiate: dAdt=2πrdrdt\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=43πr3V = \frac{4}{3} \pi r^3, so dVdt=4πr2drdt\frac{dV}{dt} = 4 \pi r^2 \frac{dr}{dt}.

Surface area: S=4πr2S = 4 \pi r^2, so dSdt=8πrdrdt\frac{dS}{dt} = 8 \pi r \frac{dr}{dt}.

Use for balloons, bubbles.

Cylinder (volume from radius and height)

If both vary: V=πr2hV = \pi r^2 h, dVdt=2πrhdrdt+πr2dhdt\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=πR23H2h3V = \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=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)V = A(h) \cdot (length), giving dVdt=\frac{dV}{dt} = (length) A(h)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=1.8sx\frac{5}{s} = \frac{1.8}{s - x}, giving 5(sx)=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=25161.2=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.

Examples in context

Example 1. Spreading oil slick. An oil slick spreads as a circle whose area grows at dAdt=8\frac{dA}{dt} = 8 m2^2/s. Since A=πr2A = \pi r^2, differentiating gives dAdt=2πrdrdt\frac{dA}{dt} = 2\pi r\frac{dr}{dt}. When the radius is r=4r = 4 m, 8=2π(4)drdt8 = 2\pi(4)\frac{dr}{dt}, so drdt=88π=1π0.318\frac{dr}{dt} = \frac{8}{8\pi} = \frac{1}{\pi} \approx 0.318 m/s.

Example 2. Draining cylindrical tank. A cylindrical tank of fixed radius 22 m drains so its volume falls at dVdt=0.6\frac{dV}{dt} = -0.6 m3^3/min. With V=πr2h=4πhV = \pi r^2 h = 4\pi h (radius fixed), differentiating gives dVdt=4πdhdt\frac{dV}{dt} = 4\pi\frac{dh}{dt}. So 0.6=4πdhdt-0.6 = 4\pi\frac{dh}{dt} and dhdt=0.64π0.0477\frac{dh}{dt} = \frac{-0.6}{4\pi} \approx -0.0477 m/min (the level falls).

Try this

Q1. A circle's radius grows at drdt=3\frac{dr}{dt} = 3 cm/s. Find the rate of area increase when r=5r = 5 cm. [3 marks]

  • Cue. dAdt=2πrdrdt=2π(5)(3)=30π94.2\frac{dA}{dt} = 2\pi r\frac{dr}{dt} = 2\pi(5)(3) = 30\pi \approx 94.2 cm2^2/s.

Q2. A spherical balloon's volume increases at 2020 cm3^3/s. Find drdt\frac{dr}{dt} when r=5r = 5 cm. [3 marks]

  • Cue. dVdt=4πr2drdt\frac{dV}{dt} = 4\pi r^2\frac{dr}{dt}; 20=100πdrdt20 = 100\pi\frac{dr}{dt}, so drdt=15π0.0637\frac{dr}{dt} = \frac{1}{5\pi} \approx 0.0637 cm/s.

Q3. A 55 m ladder slides down a wall; its foot moves out at 0.50.5 m/s. When the foot is 33 m from the wall, find the rate the top descends. [4 marks]

  • Cue. x2+y2=25x^2 + y^2 = 25, at x=3x = 3, y=4y = 4; 2xdxdt+2ydydt=02x\frac{dx}{dt} + 2y\frac{dy}{dt} = 0; dydt=3(0.5)4=0.375\frac{dy}{dt} = -\frac{3(0.5)}{4} = -0.375 m/s.

Exam-style practice questions

Practice questions written in the style of VCAA exam questions on this dot point, with worked answer explainers. The year tag is the paper they imitate, not the source.

2024 VCAA Paper 24 marksA spherical balloon is being inflated such that its volume increases at a rate of 5050 cm3^3 per second. Find the rate at which the radius is increasing when the radius is 1010 cm.
Show worked answer →

Step 1. Relate the variables. Volume of a sphere: V=43πr3V = \frac{4}{3} \pi r^3.

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

dVdt=4πr2drdt\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=4π(10)2drdt=400πdrdt50 = 4 \pi (10)^2 \cdot \frac{dr}{dt} = 400 \pi \cdot \frac{dr}{dt}.

Step 4. Solve.

drdt=50400π=18π\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 0.50.5 m3^3 per minute. Find the rate at which the water level is rising when the depth is 1 m.
Show worked answer →

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=13πr2h=13π(h2)2h=πh312V = \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=π123h2dhdt=πh24dhdt\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=π(1)24dhdt=π4dhdt0.5 = \frac{\pi (1)^2}{4} \cdot \frac{dh}{dt} = \frac{\pi}{4} \cdot \frac{dh}{dt}.

Step 4. Solve.

dhdt=0.5×4π=2π\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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