Skip to main content
QLDSpecialist MathematicsSyllabus dot point

Topic 2: Rates of change and differential equations

Model and solve practical situations with first-order differential equations, including exponential growth and decay, Newton's law of cooling and the logistic equation, and interpret the long-term behaviour of solutions

A focused answer to the QCE Specialist Mathematics Unit 4 dot point on differential equation models. Covers exponential growth and decay, Newton's law of cooling, the logistic equation and its carrying capacity, and the long-term behaviour of each model, with a verified worked example and the equilibrium-interpretation trap.

Generated by Claude Opus 4.77 min answer

Reviewed by: AI editorial process; not yet individually human-reviewed

Have a quick question? Jump to the Q&A page

What this dot point is asking

QCAA wants you to recognise the standard first-order models, set up the differential equation from a worded scenario, solve it (usually by separation of variables), apply initial conditions, and interpret long-term behaviour. The three core models are exponential growth and decay, Newton's law of cooling, and the logistic equation, each with a characteristic solution and limiting value.

The answer

Exponential growth and decay

When a quantity changes at a rate proportional to its current size,

dNdt=kNΒ β‡’Β N=N0ekt.\frac{dN}{dt} = kN \ \Rightarrow\ N = N_0 e^{kt}.

If k>0k > 0 the quantity grows without bound; if k<0k < 0 it decays toward zero. This models populations, radioactive decay and continuously compounded interest. The half-life or doubling time follows from ekte^{kt}.

Newton's law of cooling

The temperature TT of an object changes at a rate proportional to the difference from the ambient temperature TsT_s:

dTdt=βˆ’k(Tβˆ’Ts),k>0.\frac{dT}{dt} = -k(T - T_s), \qquad k > 0.

Separating variables gives the solution

T=Ts+(T0βˆ’Ts)eβˆ’kt,T = T_s + (T_0 - T_s)e^{-kt},

where T0T_0 is the initial temperature. As tβ†’βˆžt \to \infty, eβˆ’ktβ†’0e^{-kt} \to 0, so Tβ†’TsT \to T_s: the object approaches the surrounding temperature. The ambient temperature TsT_s is the equilibrium.

The logistic equation

Population growth limited by resources is modelled by

dPdt=kP(1βˆ’PM),\frac{dP}{dt} = kP\left(1 - \frac{P}{M}\right),

where MM is the carrying capacity. When PP is small the bracket is near 11 and growth is nearly exponential; as PP approaches MM the bracket approaches 00 and growth slows. The solution is the S-shaped logistic curve

P=M1+Aeβˆ’kt,A=Mβˆ’P0P0.P = \frac{M}{1 + A e^{-kt}}, \qquad A = \frac{M - P_0}{P_0}.

Long-term behaviour and equilibria

Each model has a limiting value. Exponential growth has none (it diverges); decay tends to 00; cooling tends to TsT_s; the logistic model tends to its carrying capacity MM. Equilibria are the constant solutions where the rate is zero: for the logistic equation, dPdt=0\frac{dP}{dt} = 0 at P=0P = 0 (unstable) and P=MP = M (stable).

Setting up from a scenario

Translate phrases into the equation. "Rate proportional to amount" gives dNdt=kN\frac{dN}{dt} = kN. "Rate proportional to the temperature difference" gives cooling. "Growth limited by a maximum sustainable level" signals the logistic model with MM that maximum. Then separate variables and integrate, applying the initial condition to find the constant.

Interpreting the constant kk

The constant kk sets the timescale: a larger ∣k∣|k| means faster change. Solve for kk using a second data point (for example a known value at a later time) when the scenario provides one.

Exam-style practice questions

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

2022 QCAA7 marksA research organisation plans to use a drone to drop a scientific instrument vertically from a stationary position above the ocean surface. The acceleration (m s^-2) of the falling instrument can be modelled by 9.8 - 0.1v, where v is its velocity (m s^-1). In order for the instrument sensors to activate, its speed as it hits the ocean surface must reach at least 20 m s^-1. However, if it hits with a speed above 50 m s^-1, the sensors will be damaged. Determine the range of the drone's flying height above the ocean surface to ensure that the sensors are activated but not damaged.
Show worked answer β†’

To link speed to height, write acceleration as v dv/dx = 9.8 - 0.1v (x is distance fallen). Separate variables:
x = integral of v / (9.8 - 0.1v) dv, taken from v = 0 (released at rest) up to the impact speed V.

Evaluate the integral [working]: v/(9.8 - 0.1v) = -10 - 980/(v - 98), so the antiderivative is -10v - 980 ln|v - 98|.
Between 0 and V this gives x(V) = -10V + 980 ln(98 / (98 - V)).

Lower height (impact speed 20): x = -10(20) + 980 ln(98/78) = -200 + 223.7 = 23.7 m.
Upper height (impact speed 50): x = -10(50) + 980 ln(98/48) = -500 + 699.5 = 199.5 m.

So the drone's flying height must lie between about 23.7 m and 199.5 m for the sensors to activate without being damaged. (The model has a terminal velocity of 98 m s^-1, found by setting the acceleration 9.8 - 0.1v = 0, so an impact speed of 50 m s^-1 is physically attainable.)