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Second order equations reducible by substitutionEdexcel International A Level Further Maths: Revision notes

Section 1

The idea of a substitution

Some second-order equations do not have constant coefficients, so the usual method (auxiliary equation, complementary function, particular integral) cannot be used directly. A substitution replaces either the variable xx by a new variable tt (change of independent variable) or yy by a new function zz (change of dependent variable) so that the new equation has constant coefficients. In this specification the substitution is always given. The steps are always the same:

  1. Express each derivative of yy in terms of the new variable, using the chain rule or the product rule.
  2. Substitute into the equation and simplify to a constant-coefficient equation.
  3. Solve it by the standard method.
  4. Convert back to the original variables and apply any initial or boundary conditions.
Key termssubstitutionconstant coefficients
Exam tip

Differentiate first, substitute second. Writing dydx\frac{dy}{dx} and d2ydx2\frac{d^2y}{dx^2} in the new variable on a separate line avoids most errors.

Section 2

Changing the independent variable: x = e^t

For x>0x>0 the substitution x=etx=\mathrm{e}^t (so t=ln⁡xt=\ln x) is the standard one. A dot denotes ddt\frac{d}{dt}. By the chain rule, since dtdx=1x=e−t\frac{dt}{dx}=\frac1x=\mathrm{e}^{-t}: dydx=e−ty˙,soxdydx=y˙.\frac{dy}{dx}=\mathrm{e}^{-t}\dot y,\qquad\text{so}\qquad x\frac{dy}{dx}=\dot y. For the second derivative, differentiate e−ty˙\mathrm{e}^{-t}\dot y with respect to xx, using the product rule and then the chain rule again: d2ydx2=e−tddt(e−ty˙)=e−2t(y¨−y˙),sox2d2ydx2=y¨−y˙.\frac{d^2y}{dx^2}=\mathrm{e}^{-t}\frac{d}{dt}\left(\mathrm{e}^{-t}\dot y\right)=\mathrm{e}^{-2t}\left(\ddot y-\dot y\right),\qquad\text{so}\qquad x^2\frac{d^2y}{dx^2}=\ddot y-\dot y. These two results turn any equation of the form ax2y′′+bxy′+cy=f(x)ax^2y''+bxy'+cy=f(x) (an Euler equation) into ay¨+(b−a)y˙+cy=f(et)a\ddot y+(b-a)\dot y+cy=f(\mathrm{e}^t), which has constant coefficients.

Key termsEuler equationchain rule
Common mistake

Writing d2ydx2=e−2ty¨\frac{d^2y}{dx^2}=\mathrm{e}^{-2t}\ddot y. The product rule gives an extra −y˙-\dot y because e−t\mathrm{e}^{-t} also depends on tt.

Exam tip

Remember the two shortcuts xdydx=y˙x\frac{dy}{dx}=\dot y and x2d2ydx2=y¨−y˙x^2\frac{d^2y}{dx^2}=\ddot y-\dot y, and be ready to derive them if the question says ‘show that’.

Section 3

Changing the dependent variable: y = z f(x)

Sometimes the substitution replaces yy by a product, for example y=z e−x2y=z\,\mathrm{e}^{-x^2} where zz is a new function of xx. Differentiate with the product rule and substitute. Example: with y=ze−x2y=z\mathrm{e}^{-x^2}, y′=(z′−2xz)e−x2,y′′=(z′′−4xz′+(4x2−2)z)e−x2.y'=(z'-2xz)\mathrm{e}^{-x^2},\qquad y''=\left(z''-4xz'+(4x^2-2)z\right)\mathrm{e}^{-x^2}. In y′′+4xy′+(4x2+2)yy''+4xy'+(4x^2+2)y, the z′z' terms cancel (−4xz′+4xz′-4xz'+4xz') and the zz terms give (4x2−2)−8x2+(4x2+2)=0(4x^2-2)-8x^2+(4x^2+2)=0, leaving e−x2z′′\mathrm{e}^{-x^2}z''. The equation becomes z′′=0z''=0 (or z′′=g(x)z''=g(x) if the right-hand side is non-zero), which integrates directly. Every term contains the factor e−x2\mathrm{e}^{-x^2}, which is never zero, so it can be cancelled from both sides.

Key termsproduct ruledependent variable
Common mistake

Forgetting the chain-rule factor when differentiating e−x2\mathrm{e}^{-x^2}: ddxe−x2=−2xe−x2\frac{d}{dx}\mathrm{e}^{-x^2}=-2x\mathrm{e}^{-x^2}, not −x2e−x2-x^2\mathrm{e}^{-x^2}.

Section 4

Solving the transformed equation

Once the equation has constant coefficients, solve ay¨+by˙+cy=f(t)a\ddot y+b\dot y+cy=f(t) as in FP2 5.1:

  • the auxiliary equation am2+bm+c=0am^2+bm+c=0 gives the complementary function (two real roots m1,m2m_1,m_2: Aem1t+Bem2tA\mathrm{e}^{m_1t}+B\mathrm{e}^{m_2t}; repeated root mm: (A+Bt)emt(A+Bt)\mathrm{e}^{mt}; complex roots p±iqp\pm iq: ept(Acos⁡qt+Bsin⁡qt)\mathrm{e}^{pt}(A\cos qt+B\sin qt));
  • a particular integral is chosen to match f(t)f(t); if its form already appears in the complementary function, multiply by tt (or t2t^2 for a repeated root);
  • the general solution is the complementary function plus the particular integral. Finally substitute back using t=ln⁡xt=\ln x and et=x\mathrm{e}^t=x. For example y=(A+Bt)e−2ty=(A+Bt)\mathrm{e}^{-2t} becomes y=A+Bln⁡xx2y=\frac{A+B\ln x}{x^2}.
Key termsauxiliary equationcomplementary functionparticular integral
Exam tip

If the right-hand side is 2te2t2t\mathrm{e}^{2t} and 22 is a repeated root of the auxiliary equation, the particular integral is λt3e2t\lambda t^3\mathrm{e}^{2t}, not (λt+μ)e2t(\lambda t+\mu)\mathrm{e}^{2t}.

Section 5

Initial conditions and converting back

Conditions are usually given in terms of xx, so convert them carefully.

  • A value y(x0)y(x_0) becomes yy at t0=ln⁡x0t_0=\ln x_0 (at x=1x=1, t=0t=0).
  • A condition on dydx\frac{dy}{dx} becomes a condition on y˙\dot y through y˙=xdydx\dot y=x\frac{dy}{dx}. At x=1x=1, y˙=dydx\dot y=\frac{dy}{dx}. Worked example: x2y′′+5xy′+4y=0x^2y''+5xy'+4y=0 with y(1)=1y(1)=1, y′(1)=0y'(1)=0. With x=etx=\mathrm{e}^t the equation is y¨+4y˙+4y=0\ddot y+4\dot y+4y=0, so y=(A+Bt)e−2ty=(A+Bt)\mathrm{e}^{-2t}. At t=0t=0: A=1A=1. Then y˙=(B−2A−2Bt)e−2t\dot y=(B-2A-2Bt)\mathrm{e}^{-2t}, equal to 00 at t=0t=0, so B=2B=2. Hence y=1+2ln⁡xx2y=\frac{1+2\ln x}{x^2}. Check the answer by differentiating it, or by testing the original equation at one value of xx.
Key termsinitial condition
Common mistake

Applying a condition on dydx\frac{dy}{dx} to dydt\frac{dy}{dt} without converting. Use dydt=xdydx\frac{dy}{dt}=x\frac{dy}{dx}.

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Exam questions on Second order equations reducible by substitution

  1. A differential equation for yy in terms of xx (x>0x>0) is to be transformed using the substitution x=etx=\mathrm{e}^t. A dot denotes differentiation with respect to tt, so y˙=dydt\dot y=\frac{dy}{dt} and y¨=d2ydt2\ddot y=\frac{d^2y}{dt^2}.
    The equation x2d2ydx2−2xdydx+2y=0x^2\frac{d^2y}{dx^2}-2x\frac{dy}{dx}+2y=0 transforms into y¨−3y˙+2y=0\ddot y-3\dot y+2y=0. Find the general solution for yy in terms of xx.2 marks
  2. The differential equation d2ydx2+4xdydx+(4x2+2)y=8e−x2\frac{d^2y}{dx^2}+4x\frac{dy}{dx}+(4x^2+2)y=8\mathrm{e}^{-x^2} is to be transformed using the substitution y=z e−x2y=z\,\mathrm{e}^{-x^2}, where zz is a function of xx.
    The equation transforms into d2zdx2=8\frac{d^2z}{dx^2}=8. Find the general solution for yy in terms of xx.2 marks
  3. The differential equation x2d2ydx2+5xdydx+4y=0x^2\frac{d^2y}{dx^2}+5x\frac{dy}{dx}+4y=0, x>0x>0, is to be solved using the substitution x=etx=\mathrm{e}^t.
    Show that the substitution transforms the equation into d2ydt2+4dydt+4y=0\frac{d^2y}{dt^2}+4\frac{dy}{dt}+4y=0.3 marks
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Written by the Exaim team, led by Shaun Daswani (Head of Upper Secondary, Improve ME Institute; MSc Financial Mathematics, Imperial College London; BSc, UCL) and Jason Daswani (operational lead, Improve ME Institute; LSE).