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How do we solve first-order differential equations and interpret their solutions?

Solve first-order differential equations by direct integration and by separating variables, find particular solutions from conditions, and interpret solutions in context

A focused answer to the H2 Mathematics outcome on differential equations. Solving by direct integration and separation of variables, applying boundary conditions for particular solutions, and modelling growth and decay.

Generated by Claude Opus 4.810 min answer

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

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  1. What this dot point is asking
  2. The answer
  3. Examples in context
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What this dot point is asking

SEAB wants you to solve first-order differential equations by direct integration and by separating variables, find a particular solution using a given condition, and interpret the solution in a modelling context such as growth, decay or cooling.

The answer

Direct integration

If dydx=f(x)\dfrac{dy}{dx} = \mathrm{f}(x) (the right side depends only on xx), integrate directly:

y=f(x)dx+C.y = \int \mathrm{f}(x)\,dx + C.

Separation of variables

If dydx=g(x)h(y)\dfrac{dy}{dx} = \mathrm{g}(x)\mathrm{h}(y), separate the variables to opposite sides and integrate:

1h(y)dy=g(x)dx.\int \frac{1}{\mathrm{h}(y)}\,dy = \int \mathrm{g}(x)\,dx.

This is the central technique. Treat dydx\dfrac{dy}{dx} as a ratio of differentials for the rearrangement, gather all yy with dydy and all xx with dxdx, then integrate both sides (one constant suffices).

General and particular solutions

Integration introduces an arbitrary constant, giving the general solution (a family of curves). A boundary or initial condition fixes the constant, giving the particular solution for the specific situation.

Modelling growth and decay

The equation dydt=ky\dfrac{dy}{dt} = ky (rate proportional to amount) separates to y=Aekty = Ae^{kt}: exponential growth for k>0k > 0, decay for k<0k < 0. Newton's law of cooling dθdt=k(θθs)\dfrac{d\theta}{dt} = -k(\theta - \theta_s) separates similarly, giving an exponential approach to the surrounding temperature.

Using partial fractions to separate

When separation produces a rational function of yy on the left, partial fractions often make it integrable. The logistic model dPdt=kP(1P)\dfrac{dP}{dt} = kP(1 - P) separates to 1P(1P)dP=kdt\displaystyle\int \dfrac{1}{P(1 - P)}\,dP = \int k\,dt, and the left integrand splits as 1P+11P\dfrac{1}{P} + \dfrac{1}{1 - P}, each a logarithm. This links the differential-equations work directly to the partial-fractions and integration techniques: a separable equation is only as solvable as the integrals it produces, so recognising when partial fractions are needed is part of the method.

Sketching the family of solution curves

The general solution of a first-order equation is a family of curves, one for each value of the constant, and a boundary condition selects the single curve through a given point. Sketching a few members of the family, then highlighting the particular solution, is a common H2 task that checks understanding rather than algebra. For dydx=ky\dfrac{dy}{dx} = ky, the family is a set of exponential curves y=Aekxy = Ae^{kx} of different heights, and the condition fixes which one passes through the stated point. Reading the constant as "which curve in the family" makes the general-versus-particular distinction concrete.

Examples in context

Example 1. Radioactive decay. A sample with dNdt=λN\dfrac{dN}{dt} = -\lambda N decays as N=N0eλtN = N_0 e^{-\lambda t}; the half-life follows from setting N=12N0N = \tfrac{1}{2}N_0, the standard nuclear-physics result obtained by separation of variables.

Example 2. Cooling coffee. A cup of coffee obeying Newton's law of cooling approaches room temperature exponentially, with the time constant from kk; solving the differential equation predicts the temperature at any later time.

Try this

Q1. Solve dydx=3x2\dfrac{dy}{dx} = 3x^2 with y=1y = 1 at x=0x = 0. [2 marks]

  • Cue. y=x3+Cy = x^3 + C, condition gives C=1C = 1, so y=x3+1y = x^3 + 1.

Q2. Solve dydx=ky\dfrac{dy}{dx} = ky in general form. [2 marks]

  • Cue. Separate to 1ydy=kdx\frac{1}{y}dy = k\,dx; y=Aekxy = Ae^{kx}.

Q3. State the difference between a general and a particular solution. [2 marks]

  • Cue. The general solution contains an arbitrary constant (a family of curves); the particular solution fixes it using a given condition.

Exam-style practice questions

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

Original5 marksSolve the differential equation dydx=2xy\dfrac{dy}{dx} = \dfrac{2x}{y}, given that y=3y = 3 when x=0x = 0.
Show worked answer →

Separate variables: ydy=2xdxy\,dy = 2x\,dx.

Integrate: y22=x2+C\dfrac{y^2}{2} = x^2 + C.

Apply the condition y=3y = 3, x=0x = 0: 92=0+C\dfrac{9}{2} = 0 + C, so C=92C = \dfrac{9}{2}.

Hence y22=x2+92\dfrac{y^2}{2} = x^2 + \dfrac{9}{2}, that is y2=2x2+9y^2 = 2x^2 + 9, so y=2x2+9y = \sqrt{2x^2 + 9} (positive root since y=3>0y = 3 > 0).

Markers reward separating the variables, integrating both sides, applying the condition for CC, and the explicit solution with the correct sign.

Original6 marksA population PP grows according to dPdt=kP\dfrac{dP}{dt} = kP, where kk is a positive constant. Solve the equation and, given that P=1000P = 1000 at t=0t = 0 and P=1500P = 1500 at t=2t = 2, find kk.
Show worked answer →

Separate: 1PdP=kdt\dfrac{1}{P}\,dP = k\,dt. Integrate: lnP=kt+C\ln P = kt + C, so P=AektP = Ae^{kt} where A=eCA = e^C.

At t=0t = 0, P=1000P = 1000, so A=1000A = 1000, giving P=1000ektP = 1000e^{kt}.

At t=2t = 2, P=1500P = 1500: 1500=1000e2k1500 = 1000e^{2k}, so e2k=1.5e^{2k} = 1.5, 2k=ln1.52k = \ln 1.5, k=12ln1.50.203k = \dfrac{1}{2}\ln 1.5 \approx 0.203.

Markers reward separating, integrating to the exponential form, finding AA from the initial condition, and solving for kk with logarithms.

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