FP1-3 Further differential equations (Further Pure 1) — revision question pack

2 specification points · notes, questions, answers and worked methods

Checked against Edexcel 9FM0 section FP1-3. Review basis: the qualification registry sourced from the Pearson Edexcel Level 3 Advanced GCE in Further Mathematics (9FM0) specification; registry verification recorded 17 July 2026.

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FP1-3.1 · Use of Taylor series method for series solution of differential equations.

Explanation

  • When a differential equation cannot be solved in closed form, a Taylor series about the point where the initial conditions are given still produces a usable local solution. The method is mechanical:
  • substitute the initial values into the equation to get the first unknown derivative, differentiate the whole equation with respect to xx, substitute again, and repeat until you have every derivative you need.
  • Assemble them with y=y(a)+y(a)(xa)+y(a)2!(xa)2+y=y(a)+y'(a)(x-a)+\dfrac{y''(a)}{2!}(x-a)^2+\cdots. For a first-order equation y=f(x,y)y'=f(x,y) you differentiate ff using the chain rule, remembering that yy is a function of xx, so ddx(y2)=2yy\dfrac{\mathrm{d}}{\mathrm{d}x}\left(y^2\right)=2yy'.
  • For a second-order equation both y(a)y(a) and y(a)y'(a) are given and the equation supplies y(a)y''(a) directly.
  • Keep a running table of the values at x=ax=a; that table, not the algebra, is what you assemble the series from.

Worked example

Find the series solution in ascending powers of xx, as far as the term in x4x^4, of d2ydx2+xdydx+y=0\dfrac{\mathrm{d}^2y}{\mathrm{d}x^2}+x\dfrac{\mathrm{d}y}{\mathrm{d}x}+y=0, given that y=0y=0 and dydx=1\dfrac{\mathrm{d}y}{\mathrm{d}x}=1 at x=0x=0.

  1. 1.Rearranged, y=xyyy''=-xy'-y, so at x=0x=0, y=00=0y''=0-0=0.
  2. 2.Differentiating, y=2yxyy'''=-2y'-xy'', so y(0)=2y'''(0)=-2.
  3. 3.Differentiating again, y(4)=3yxyy^{(4)}=-3y''-xy''', so y(4)(0)=0y^{(4)}(0)=0.
  4. 4.Assembling: y=0+x+02x36+0=xx33y=0+x+0-\dfrac{2x^3}{6}+0=x-\dfrac{x^3}{3}.

Answer: y=xx33+y=x-\dfrac{x^3}{3}+\cdots, with the x2x^2 and x4x^4 terms both zero.

Common mistakes

  • Don't fall into the trap of differentiating y2y^2 as 2y2y instead of 2yy2yy'.
  • Don't fall into the trap of substituting x=0x=0 before differentiating the whole equation, which destroys the terms needed next.
  • Don't fall into the trap of dividing the derivative values by nn rather than n!n! when assembling the series.

Exam tip

Never substitute the initial values into an expression you still need to differentiate; keep one general line and one numerical line side by side.

Tier 1 · Easy

  1. 1.

    Given that dydx=x+y\dfrac{\mathrm{d}y}{\mathrm{d}x}=x+y and y=1y=1 at x=0x=0, find the series solution for yy in ascending powers of xx as far as the term in x3x^3.

    (4)

    (Total for Question 1 is 4 marks)

  2. 2.

    Given that dydx=y2\dfrac{\mathrm{d}y}{\mathrm{d}x}=y^2 and y=1y=1 at x=0x=0, find the series solution for yy as far as the term in x3x^3.

    (4)

    (Total for Question 2 is 4 marks)

Tier 2 · Standard

  1. 1.

    Given that dydx=x2+y2\dfrac{\mathrm{d}y}{\mathrm{d}x}=x^2+y^2 and y=1y=1 at x=0x=0, find the series solution for yy as far as the term in x4x^4.

    (6)

    (Total for Question 1 is 6 marks)

  2. 2.

    Given that d2ydx2=dydx+2y\dfrac{\mathrm{d}^2y}{\mathrm{d}x^2}=\dfrac{\mathrm{d}y}{\mathrm{d}x}+2y with y=1y=1 and dydx=0\dfrac{\mathrm{d}y}{\mathrm{d}x}=0 at x=0x=0, find the series solution as far as the term in x4x^4.

    (6)

    (Total for Question 2 is 6 marks)

  3. 3.

    Given that d2ydx2=xdydx+y\dfrac{\mathrm{d}^2y}{\mathrm{d}x^2}=x\dfrac{\mathrm{d}y}{\mathrm{d}x}+y with y=1y=1 and dydx=1\dfrac{\mathrm{d}y}{\mathrm{d}x}=1 at x=0x=0, find the series solution as far as the term in x5x^5.

    (6)

    (Total for Question 3 is 6 marks)

Tier 3 · Hard

  1. 1.

    Given that dydx=sin(x+y)\dfrac{\mathrm{d}y}{\mathrm{d}x}=\sin(x+y) and y=0y=0 at x=0x=0, find the series solution for yy as far as the term in x3x^3.

    (6)

    (Total for Question 1 is 6 marks)

  2. 2.

    Given that dydx=x+y2\dfrac{\mathrm{d}y}{\mathrm{d}x}=x+y^2 and y=0y=0 at x=0x=0, find the series solution for yy as far as the term in x5x^5.

    (6)

    (Total for Question 2 is 6 marks)

  3. 3.

    Given that d2ydx2=y2+x\dfrac{\mathrm{d}^2y}{\mathrm{d}x^2}=y^2+x with y=1y=1 and dydx=0\dfrac{\mathrm{d}y}{\mathrm{d}x}=0 at x=0x=0, find the series solution as far as the term in x4x^4.

    (6)

    (Total for Question 3 is 6 marks)

  4. 4.

    Given that dydx=xy2\dfrac{\mathrm{d}y}{\mathrm{d}x}=x-y^2 and y=2y=2 at x=1x=1, find the series solution for yy in ascending powers of (x1)(x-1) as far as the term in (x1)3(x-1)^3.

    (6)

    (Total for Question 4 is 6 marks)

  5. 5.

    Using the series solution y=23(x1)+132(x1)2353(x1)3y=2-3(x-1)+\dfrac{13}{2}(x-1)^2-\dfrac{35}{3}(x-1)^3 of dydx=xy2\dfrac{\mathrm{d}y}{\mathrm{d}x}=x-y^2 with y(1)=2y(1)=2, estimate y(1.1)y(1.1) to 44 decimal places and comment on the accuracy of the estimate.

    (5)

    (Total for Question 5 is 5 marks)

FP1-3.2 · Differential equations reducible by means of a given substitution.

Explanation

  • The question always supplies the substitution; your job is to carry it through correctly and land on one of the standard forms from Core Pure section 9 — a first-order linear equation solved by an integrating factor, a separable equation, or a second-order linear equation with constant coefficients. Three patterns dominate.
  • First, z=y1nz=y^{1-n} turns y+P(x)y=Q(x)yny'+P(x)y=Q(x)y^{n} into a linear equation in zz; the working starts by dividing through by yny^{n}.
  • Second, y=vxy=vx turns a homogeneous equation into a separable one in vv and xx, using dydx=v+xdvdx\dfrac{\mathrm{d}y}{\mathrm{d}x}=v+x\dfrac{\mathrm{d}v}{\mathrm{d}x}.
  • Third, x=eux=\mathrm{e}^{u} turns an Euler equation into constant coefficients, using xdydx=dydux\dfrac{\mathrm{d}y}{\mathrm{d}x}=\dfrac{\mathrm{d}y}{\mathrm{d}u} and x2d2ydx2=d2ydu2dydux^2\dfrac{\mathrm{d}^2y}{\mathrm{d}x^2}=\dfrac{\mathrm{d}^2y}{\mathrm{d}u^2}-\dfrac{\mathrm{d}y}{\mathrm{d}u}.
  • Always convert the final answer back to the original variables, and apply any boundary condition only after that conversion.

Worked example

Use the substitution z=y2z=y^{2} to solve 2ydydx+y2=x2y\dfrac{\mathrm{d}y}{\mathrm{d}x}+y^{2}=x.

  1. 1.z=y2z=y^2 gives dzdx=2ydydx\dfrac{\mathrm{d}z}{\mathrm{d}x}=2y\dfrac{\mathrm{d}y}{\mathrm{d}x}, so the equation becomes dzdx+z=x\dfrac{\mathrm{d}z}{\mathrm{d}x}+z=x.
  2. 2.The integrating factor is ex\mathrm{e}^{x}, so ddx(zex)=xex\dfrac{\mathrm{d}}{\mathrm{d}x}\left(z\mathrm{e}^{x}\right)=x\mathrm{e}^{x}.
  3. 3.Integrating by parts, zex=(x1)ex+Az\mathrm{e}^{x}=(x-1)\mathrm{e}^{x}+A, so z=x1+Aexz=x-1+A\mathrm{e}^{-x}.

Answer: y2=x1+Aexy^{2}=x-1+A\mathrm{e}^{-x}.

Common mistakes

  • Don't fall into the trap of failing to divide through by yny^{n} before substituting in a Bernoulli equation, so the new variable never appears cleanly.
  • Don't fall into the trap of using dydx=xdvdx\dfrac{\mathrm{d}y}{\mathrm{d}x}=x\dfrac{\mathrm{d}v}{\mathrm{d}x} instead of v+xdvdxv+x\dfrac{\mathrm{d}v}{\mathrm{d}x} for y=vxy=vx.
  • Don't fall into the trap of leaving the answer in terms of the substituted variable instead of returning to yy and xx.

Exam tip

Write the derivative of the substitution on its own line before touching the equation; almost every lost mark in this topic comes from that one differentiation.

Tier 1 · Easy

  1. 1.

    Use the substitution z=y1z=y^{-1} to show that dydx+y=xy2\dfrac{\mathrm{d}y}{\mathrm{d}x}+y=xy^{2} reduces to dzdxz=x\dfrac{\mathrm{d}z}{\mathrm{d}x}-z=-x.

    (3)

    (Total for Question 1 is 3 marks)

  2. 2.

    Use the substitution y=vxy=vx to show that xdydx=y+xtanyxx\dfrac{\mathrm{d}y}{\mathrm{d}x}=y+x\tan\dfrac{y}{x} reduces to xdvdx=tanvx\dfrac{\mathrm{d}v}{\mathrm{d}x}=\tan v.

    (3)

    (Total for Question 2 is 3 marks)

Tier 2 · Standard

  1. 1.

    Use the substitution z=y1z=y^{-1} to find the general solution of dydx+y=xy2\dfrac{\mathrm{d}y}{\mathrm{d}x}+y=xy^{2}.

    (6)

    (Total for Question 1 is 6 marks)

  2. 2.

    Use the substitution x=eux=\mathrm{e}^{u} to find the general solution of x2d2ydx2+xdydx4y=0x^{2}\dfrac{\mathrm{d}^{2}y}{\mathrm{d}x^{2}}+x\dfrac{\mathrm{d}y}{\mathrm{d}x}-4y=0 for x>0x>0.

    (6)

    (Total for Question 2 is 6 marks)

  3. 3.

    Use the substitution u=dydxu=\dfrac{\mathrm{d}y}{\mathrm{d}x} to find the general solution of xd2ydx2+dydx=xx\dfrac{\mathrm{d}^{2}y}{\mathrm{d}x^{2}}+\dfrac{\mathrm{d}y}{\mathrm{d}x}=x for x>0x>0.

    (6)

    (Total for Question 3 is 6 marks)

Tier 3 · Hard

  1. 1.

    Use the substitution y=vxy=vx to solve dydx=x2+y2xy\dfrac{\mathrm{d}y}{\mathrm{d}x}=\dfrac{x^{2}+y^{2}}{xy} given that y=2y=2 when x=1x=1, and express yy in terms of xx.

    (7)

    (Total for Question 1 is 7 marks)

  2. 2.

    Use the substitution z=sinyz=\sin y to find the general solution of cosydydx+sinyx=x\cos y\dfrac{\mathrm{d}y}{\mathrm{d}x}+\dfrac{\sin y}{x}=x for x>0x>0.

    (7)

    (Total for Question 2 is 7 marks)

  3. 3.

    Use the substitution u=xyu=xy to find the general solution of xd2ydx2+2dydx+xy=0x\dfrac{\mathrm{d}^{2}y}{\mathrm{d}x^{2}}+2\dfrac{\mathrm{d}y}{\mathrm{d}x}+xy=0 for x>0x>0.

    (7)

    (Total for Question 3 is 7 marks)

  4. 4.

    Use the substitution u=dydxu=\dfrac{\mathrm{d}y}{\mathrm{d}x} to solve d2ydx2=1+(dydx)2\dfrac{\mathrm{d}^{2}y}{\mathrm{d}x^{2}}=1+\left(\dfrac{\mathrm{d}y}{\mathrm{d}x}\right)^{2} given that y=0y=0 and dydx=0\dfrac{\mathrm{d}y}{\mathrm{d}x}=0 at x=0x=0.

    (7)

    (Total for Question 4 is 7 marks)

  5. 5.

    Use the substitution x=eux=\mathrm{e}^{u} to find the general solution of x2d2ydx23xdydx+4y=x2x^{2}\dfrac{\mathrm{d}^{2}y}{\mathrm{d}x^{2}}-3x\dfrac{\mathrm{d}y}{\mathrm{d}x}+4y=x^{2} for x>0x>0.

    (8)

    (Total for Question 5 is 8 marks)

Answer key

Answers begin on a new printed page so the question pack can be completed without the solutions alongside it.

FP1-3.1 · Use of Taylor series method for series solution of differential equations.

Tier 1 · Easy

Mark scheme for FP1-3.1 Tier 1 · Easy
QuestionSchemeMarks
1
  • y(0)=0+1=1y'(0)=0+1=1
  • y=1+yy''=1+y' so y(0)=2y''(0)=2; y=yy'''=y'' so y(0)=2y'''(0)=2
  • y=1+x+x2+x33+y=1+x+x^2+\dfrac{x^3}{3}+\cdots
4
(4 marks)4
Notes
Substituting gives y(0)=1y'(0)=1; differentiating the equation gives y=1+yy''=1+y' and y=yy'''=y'', so the values at 00 are 22 and 22, and the coefficients are 22!=1\tfrac{2}{2!}=1 and 23!=13\tfrac{2}{3!}=\tfrac13. Independent check: the exact solution is y=2exx1y=2\mathrm{e}^{x}-x-1, whose expansion is 2(1+x+x22+x36)x1=1+x+x2+x332\left(1+x+\tfrac{x^2}{2}+\tfrac{x^3}{6}\right)-x-1=1+x+x^2+\tfrac{x^3}{3}.
2
  • y(0)=1y'(0)=1
  • y=2yyy''=2yy' so y(0)=2y''(0)=2
  • y=2(y)2+2yyy'''=2\left(y'\right)^2+2yy'' so y(0)=2+4=6y'''(0)=2+4=6
  • y=1+x+x2+x3+y=1+x+x^2+x^3+\cdots
4
(4 marks)4
Notes
Differentiating with the chain rule gives y=2yyy''=2yy' and y=2(y)2+2yyy'''=2(y')^2+2yy'', with values 22 and 66 at x=0x=0; dividing by 2!2! and 3!3! gives coefficients 11 and 11. Independent check: separating variables gives y=11xy=\dfrac1{1-x}, whose binomial expansion is 1+x+x2+x3+1+x+x^2+x^3+\cdots.

Tier 2 · Standard

Mark scheme for FP1-3.1 Tier 2 · Standard
QuestionSchemeMarks
1
  • y(0)=1y'(0)=1
  • y=2x+2yyy''=2x+2yy' so y(0)=2y''(0)=2
  • y=2+2(y)2+2yyy'''=2+2\left(y'\right)^2+2yy'' so y(0)=8y'''(0)=8
  • y(4)=6yy+2yyy^{(4)}=6y'y''+2yy''' so y(4)(0)=12+16=28y^{(4)}(0)=12+16=28
  • y=1+x+x2+4x33+7x46+y=1+x+x^2+\dfrac{4x^3}{3}+\dfrac{7x^4}{6}+\cdots
6
(6 marks)6
Notes
Each differentiation uses the chain rule on y2y^2, giving the derivative values 1,2,8,281,2,8,28 at x=0x=0; dividing by 2!,3!,4!2!,3!,4! gives 11, 86=43\tfrac86=\tfrac43 and 2824=76\tfrac{28}{24}=\tfrac76. Independent check by fourth-order numerical integration with step 10610^{-6}: the solution at x=0.1x=0.1 is 1.1114631.111463, and the series gives 1+0.1+0.01+0.001333+0.000117=1.1114501+0.1+0.01+0.001333+0.000117=1.111450, agreeing to the order of the first neglected term.
2
  • y(0)=0+2=2y''(0)=0+2=2
  • y=y+2yy'''=y''+2y' so y(0)=2y'''(0)=2
  • y(4)=y+2yy^{(4)}=y'''+2y'' so y(4)(0)=6y^{(4)}(0)=6
  • y=1+x2+x33+x44+y=1+x^2+\dfrac{x^3}{3}+\dfrac{x^4}{4}+\cdots
6
(6 marks)6
Notes
The equation gives y(0)=2y''(0)=2 directly, and each further differentiation reuses the same relation, giving 22 and 66. Independent check: the auxiliary equation m2m2=0m^2-m-2=0 has roots 22 and 1-1, so y=13e2x+23exy=\tfrac13\mathrm{e}^{2x}+\tfrac23\mathrm{e}^{-x}, whose expansion is 1+x2+x33+x44+1+x^2+\tfrac{x^3}{3}+\tfrac{x^4}{4}+\cdots.
3
  • y(0)=0+1=1y''(0)=0+1=1
  • y=2y+xyy'''=2y'+xy'' so y(0)=2y'''(0)=2
  • y(4)=3y+xyy^{(4)}=3y''+xy''' so y(4)(0)=3y^{(4)}(0)=3
  • y(5)=4y+xy(4)y^{(5)}=4y'''+xy^{(4)} so y(5)(0)=8y^{(5)}(0)=8
  • y=1+x+x22+x33+x48+x515+y=1+x+\dfrac{x^2}{2}+\dfrac{x^3}{3}+\dfrac{x^4}{8}+\dfrac{x^5}{15}+\cdots
6
(6 marks)6
Notes
Differentiating the product xyxy' each time raises the coefficient by one, giving the pattern y(n+2)=ny(n)+y^{(n+2)}=ny^{(n)}+\cdots and the values 1,2,3,81,2,3,8. Dividing by the factorials gives 12\tfrac12, 26=13\tfrac26=\tfrac13, 324=18\tfrac3{24}=\tfrac18 and 8120=115\tfrac8{120}=\tfrac1{15}. Independent check: the values satisfy the equation term by term, since substituting the series into yxyyy''-xy'-y makes every coefficient up to x3x^3 vanish.

Tier 3 · Hard

Mark scheme for FP1-3.1 Tier 3 · Hard
QuestionSchemeMarks
1
  • y(0)=sin0=0y'(0)=\sin0=0
  • y=cos(x+y)(1+y)y''=\cos(x+y)\left(1+y'\right) so y(0)=1y''(0)=1
  • y=sin(x+y)(1+y)2+cos(x+y)yy'''=-\sin(x+y)\left(1+y'\right)^2+\cos(x+y)y'' so y(0)=1y'''(0)=1
  • y=x22+x36+y=\dfrac{x^2}{2}+\dfrac{x^3}{6}+\cdots
6
(6 marks)6
Notes
Differentiating sin(x+y)\sin(x+y) requires the chain rule with inner derivative 1+y1+y', and the second differentiation needs the product rule as well. Independent check by fourth-order numerical integration with step 10410^{-4}: at x=0.2x=0.2 the numerical solution is 0.0213140.021314, and the series gives 0.02+0.001333=0.0213330.02+0.001333=0.021333.
2
  • y(0)=0y'(0)=0 and y=1+2yyy''=1+2yy' so y(0)=1y''(0)=1
  • y=2(y)2+2yyy'''=2\left(y'\right)^2+2yy'' so y(0)=0y'''(0)=0
  • y(4)=6yy+2yyy^{(4)}=6y'y''+2yy''' so y(4)(0)=0y^{(4)}(0)=0
  • y(5)=6(y)2+8yy+2yy(4)y^{(5)}=6\left(y''\right)^2+8y'y'''+2yy^{(4)} so y(5)(0)=6y^{(5)}(0)=6
  • y=x22+x520+y=\dfrac{x^2}{2}+\dfrac{x^5}{20}+\cdots
6
(6 marks)6
Notes
Because y(0)=y(0)=0y(0)=y'(0)=0, every term containing yy or yy' vanishes at the origin until the square of yy'' appears at the fifth derivative, where 6(y)2=66\left(y''\right)^2=6. Dividing by 5!5! gives 6120=120\tfrac6{120}=\tfrac1{20}. Independent check by substituting y=x22+cx5y=\tfrac{x^2}{2}+cx^5 into the equation: the left side is x+5cx4x+5cx^4 and the right side is x+x44x+\tfrac{x^4}{4}, so c=120c=\tfrac1{20}.
3
  • y(0)=1+0=1y''(0)=1+0=1
  • y=2yy+1y'''=2yy'+1 so y(0)=1y'''(0)=1
  • y(4)=2(y)2+2yyy^{(4)}=2\left(y'\right)^2+2yy'' so y(4)(0)=2y^{(4)}(0)=2
  • y=1+x22+x36+x412+y=1+\dfrac{x^2}{2}+\dfrac{x^3}{6}+\dfrac{x^4}{12}+\cdots
6
(6 marks)6
Notes
The equation gives y(0)=1y''(0)=1; differentiating gives y=2yy+1y'''=2yy'+1 and y(4)=2(y)2+2yyy^{(4)}=2(y')^2+2yy'', with values 11 and 22 at the origin. Dividing by 3!3! and 4!4! gives 16\tfrac16 and 224=112\tfrac2{24}=\tfrac1{12}. Independent check by substitution: with y=1+x22+x36+x412y=1+\tfrac{x^2}{2}+\tfrac{x^3}{6}+\tfrac{x^4}{12}, the left side is 1+x+x2+1+x+x^2+\cdots and y2+x=1+x+x2+y^2+x=1+x+x^2+\cdots, matching to the order retained.
4
  • y(1)=14=3y'(1)=1-4=-3
  • y=12yyy''=1-2yy' so y(1)=1+12=13y''(1)=1+12=13
  • y=2(y)22yyy'''=-2\left(y'\right)^2-2yy'' so y(1)=1852=70y'''(1)=-18-52=-70
  • y=23(x1)+132(x1)2353(x1)3+y=2-3(x-1)+\dfrac{13}{2}(x-1)^2-\dfrac{35}{3}(x-1)^3+\cdots
6
(6 marks)6
Notes
Substituting the initial values gives y(1)=3y'(1)=-3; two further differentiations give 1313 and 70-70, and dividing by 2!2! and 3!3! gives 132\tfrac{13}{2} and 706=353-\tfrac{70}{6}=-\tfrac{35}{3}. Independent check: the recurrence values reproduce the equation when the series is substituted, and each coefficient alternates in sign as the y2-y^2 term dominates.
5
  • With x1=0.1x-1=0.1 the terms are 22, 0.3-0.3, 0.0650.065 and 0.0116667-0.0116667
  • y(1.1)1.7533y(1.1)\approx1.7533
  • A fourth-degree term would be needed for greater accuracy
  • The terms are not yet decreasing quickly, so the estimate is reliable only to about 22 decimal places
5
(5 marks)5
Notes
Substituting x1=0.1x-1=0.1 gives 20.3+0.0650.0116667=1.75333332-0.3+0.065-0.0116667=1.7533333, that is 1.75331.7533 to 44 decimal places. Independent check by fourth-order numerical integration of the same initial-value problem with step 10510^{-5}: y(1.1)=1.7551y(1.1)=1.7551, so the truncated series is in error by about 0.00180.0018, consistent with the size of the omitted quartic term and confirming that only about two decimal places are trustworthy.

FP1-3.2 · Differential equations reducible by means of a given substitution.

Tier 1 · Easy

Mark scheme for FP1-3.2 Tier 1 · Easy
QuestionSchemeMarks
1
  • Dividing by y2y^2 gives y2dydx+y1=xy^{-2}\dfrac{\mathrm{d}y}{\mathrm{d}x}+y^{-1}=x
  • z=y1z=y^{-1} gives dzdx=y2dydx\dfrac{\mathrm{d}z}{\mathrm{d}x}=-y^{-2}\dfrac{\mathrm{d}y}{\mathrm{d}x}
  • Substituting gives dzdx+z=x-\dfrac{\mathrm{d}z}{\mathrm{d}x}+z=x, that is dzdxz=x\dfrac{\mathrm{d}z}{\mathrm{d}x}-z=-x
3
(3 marks)3
Notes
Divide the Bernoulli equation by y2y^2 so that the combination y2yy^{-2}y' appears, then replace it by z-z' and y1y^{-1} by zz. Independent check: reversing the substitution in zz=xz'-z=-x gives y2yy1=x-y^{-2}y'-y^{-1}=-x, and multiplying by y2-y^2 returns the original equation.
2
  • y=vxy=vx gives dydx=v+xdvdx\dfrac{\mathrm{d}y}{\mathrm{d}x}=v+x\dfrac{\mathrm{d}v}{\mathrm{d}x}
  • The equation becomes x(v+xdvdx)=vx+xtanvx\left(v+x\dfrac{\mathrm{d}v}{\mathrm{d}x}\right)=vx+x\tan v
  • Cancelling vxvx and dividing by xx gives xdvdx=tanvx\dfrac{\mathrm{d}v}{\mathrm{d}x}=\tan v
3
(3 marks)3
Notes
The product rule gives y=v+xvy'=v+xv', and yx=v\tfrac{y}{x}=v, so the right side is vx+xtanvvx+x\tan v; the vxvx terms cancel and one factor of xx divides out. Independent check: the reduced equation separates as cotvdv=dxx\cot v\,\mathrm{d}v=\tfrac{\mathrm{d}x}{x}, giving lnsinv=lnx+c\ln|\sin v|=\ln|x|+c, so sinyx=Ax\sin\tfrac{y}{x}=Ax, and differentiating that implicitly returns the original equation.

Tier 2 · Standard

Mark scheme for FP1-3.2 Tier 2 · Standard
QuestionSchemeMarks
1
  • The equation becomes dzdxz=x\dfrac{\mathrm{d}z}{\mathrm{d}x}-z=-x
  • The integrating factor is ex\mathrm{e}^{-x}
  • zex=xexdx=(x+1)ex+Az\mathrm{e}^{-x}=-\displaystyle\int x\mathrm{e}^{-x}\,\mathrm{d}x=(x+1)\mathrm{e}^{-x}+A
  • z=x+1+Aexz=x+1+A\mathrm{e}^{x}
  • y=1x+1+Aexy=\dfrac{1}{x+1+A\mathrm{e}^{x}}
6
(6 marks)6
Notes
After the Bernoulli reduction the integrating factor ex\mathrm{e}^{-x} gives (zex)=xex\left(z\mathrm{e}^{-x}\right)'=-x\mathrm{e}^{-x}, and integrating by parts gives (x+1)ex+A(x+1)\mathrm{e}^{-x}+A. Independent check by substitution: with y=(x+1+Aex)1y=\left(x+1+A\mathrm{e}^{x}\right)^{-1}, y=(1+Aex)y2y'=-\left(1+A\mathrm{e}^{x}\right)y^2, so y+yxy2=y2[1Aex+x+1+Aexx]=0y'+y-xy^2=y^2\left[-1-A\mathrm{e}^{x}+x+1+A\mathrm{e}^{x}-x\right]=0.
2
  • xdydx=dydux\dfrac{\mathrm{d}y}{\mathrm{d}x}=\dfrac{\mathrm{d}y}{\mathrm{d}u} and x2d2ydx2=d2ydu2dydux^{2}\dfrac{\mathrm{d}^{2}y}{\mathrm{d}x^{2}}=\dfrac{\mathrm{d}^{2}y}{\mathrm{d}u^{2}}-\dfrac{\mathrm{d}y}{\mathrm{d}u}
  • The equation becomes d2ydu24y=0\dfrac{\mathrm{d}^{2}y}{\mathrm{d}u^{2}}-4y=0
  • The auxiliary equation m24=0m^{2}-4=0 gives m=±2m=\pm2
  • y=Ae2u+Be2uy=A\mathrm{e}^{2u}+B\mathrm{e}^{-2u}
  • y=Ax2+Bx2y=Ax^{2}+\dfrac{B}{x^{2}}
6
(6 marks)6
Notes
Substituting the two standard Euler identities cancels the first-derivative terms, leaving yuu4y=0y_{uu}-4y=0 with solution Ae2u+Be2uA\mathrm{e}^{2u}+B\mathrm{e}^{-2u}; since eu=x\mathrm{e}^{u}=x this is Ax2+Bx2Ax^2+Bx^{-2}. Independent check by direct substitution: for y=xky=x^{k} the equation gives k(k1)+k4=k24=0k(k-1)+k-4=k^2-4=0, so k=±2k=\pm2, matching the two basis solutions.
3
  • The equation becomes xdudx+u=xx\dfrac{\mathrm{d}u}{\mathrm{d}x}+u=x, that is ddx(xu)=x\dfrac{\mathrm{d}}{\mathrm{d}x}(xu)=x
  • xu=x22+Axu=\dfrac{x^{2}}{2}+A, so u=x2+Axu=\dfrac{x}{2}+\dfrac{A}{x}
  • Integrating, y=x24+Alnx+By=\dfrac{x^{2}}{4}+A\ln x+B
6
(6 marks)6
Notes
Reducing the order turns the equation into a first-order linear equation whose left side is already the exact derivative of xuxu. Integrating twice gives the general solution with two arbitrary constants. Independent check by substitution: for y=x24+Alnx+By=\tfrac{x^2}{4}+A\ln x+B, y=x2+Axy'=\tfrac{x}{2}+\tfrac{A}{x} and y=12Ax2y''=\tfrac12-\tfrac{A}{x^2}, so xy+y=x2Ax+x2+Ax=xxy''+y'=\tfrac{x}{2}-\tfrac{A}{x}+\tfrac{x}{2}+\tfrac{A}{x}=x.

Tier 3 · Hard

Mark scheme for FP1-3.2 Tier 3 · Hard
QuestionSchemeMarks
1
  • v+xdvdx=1+v2vv+x\dfrac{\mathrm{d}v}{\mathrm{d}x}=\dfrac{1+v^{2}}{v}
  • xdvdx=1vx\dfrac{\mathrm{d}v}{\mathrm{d}x}=\dfrac{1}{v}, so vdv=dxxv\,\mathrm{d}v=\dfrac{\mathrm{d}x}{x}
  • v22=lnx+c\dfrac{v^{2}}{2}=\ln x+c
  • y=2y=2 at x=1x=1 gives v=2v=2 and c=2c=2
  • y2=2x2(lnx+2)y^{2}=2x^{2}\left(\ln x+2\right)
7
(7 marks)7
Notes
Dividing numerator and denominator by x2x^2 shows the equation is homogeneous; the substitution reduces it to the separable form vdv=dxxv\,\mathrm{d}v=\tfrac{\mathrm{d}x}{x}. Applying the condition after returning to yy and xx gives c=2c=2. Independent check by differentiating the answer implicitly: 2yy=4x(lnx+2)+2x2yy'=4x(\ln x+2)+2x, so y=2xlnx+5xyy'=\dfrac{2x\ln x+5x}{y}, and substituting y2=2x2lnx+4x2y^2=2x^2\ln x+4x^2 into x2+y2xy\dfrac{x^2+y^2}{xy} gives 5x2+2x2lnxxy\dfrac{5x^2+2x^2\ln x}{xy}, the same expression.
2
  • z=sinyz=\sin y gives dzdx=cosydydx\dfrac{\mathrm{d}z}{\mathrm{d}x}=\cos y\dfrac{\mathrm{d}y}{\mathrm{d}x}
  • The equation becomes dzdx+zx=x\dfrac{\mathrm{d}z}{\mathrm{d}x}+\dfrac{z}{x}=x
  • The integrating factor is xx, so ddx(xz)=x2\dfrac{\mathrm{d}}{\mathrm{d}x}(xz)=x^{2}
  • xz=x33+Axz=\dfrac{x^{3}}{3}+A, so z=x23+Axz=\dfrac{x^{2}}{3}+\dfrac{A}{x}
  • siny=x23+Ax\sin y=\dfrac{x^{2}}{3}+\dfrac{A}{x}
7
(7 marks)7
Notes
The substitution converts the equation into a first-order linear equation in zz with integrating factor e1/xdx=x\mathrm{e}^{\int1/x\,\mathrm{d}x}=x. Independent check by differentiating the answer: from xsiny=x33+Ax\sin y=\tfrac{x^3}{3}+A, differentiating gives siny+xcosyy=x2\sin y+x\cos y\,y'=x^2, and dividing by xx returns the original equation.
3
  • u=xyu=xy gives dudx=y+xdydx\dfrac{\mathrm{d}u}{\mathrm{d}x}=y+x\dfrac{\mathrm{d}y}{\mathrm{d}x}
  • d2udx2=2dydx+xd2ydx2\dfrac{\mathrm{d}^{2}u}{\mathrm{d}x^{2}}=2\dfrac{\mathrm{d}y}{\mathrm{d}x}+x\dfrac{\mathrm{d}^{2}y}{\mathrm{d}x^{2}}
  • The equation is therefore d2udx2+u=0\dfrac{\mathrm{d}^{2}u}{\mathrm{d}x^{2}}+u=0
  • u=Acosx+Bsinxu=A\cos x+B\sin x
  • y=Acosx+Bsinxxy=\dfrac{A\cos x+B\sin x}{x}
7
(7 marks)7
Notes
Differentiating u=xyu=xy twice reproduces exactly the combination xy+2yxy''+2y', so the equation becomes simple harmonic in uu. Independent check by substitution: for y=sinxxy=\dfrac{\sin x}{x}, xy=sinxxy=\sin x, and d2dx2(sinx)+sinx=0\dfrac{\mathrm{d}^2}{\mathrm{d}x^2}(\sin x)+\sin x=0, so the original equation is satisfied.
4
  • dudx=1+u2\dfrac{\mathrm{d}u}{\mathrm{d}x}=1+u^{2}, which separates as du1+u2=dx\dfrac{\mathrm{d}u}{1+u^{2}}=\mathrm{d}x
  • arctanu=x+c\arctan u=x+c, and u=0u=0 at x=0x=0 gives c=0c=0
  • dydx=tanx\dfrac{\mathrm{d}y}{\mathrm{d}x}=\tan x
  • y=lncosx+dy=-\ln|\cos x|+d, and y=0y=0 at x=0x=0 gives d=0d=0
  • y=ln(cosx)y=-\ln(\cos x) for x<π2|x|<\dfrac{\pi}{2}
7
(7 marks)7
Notes
Reducing the order gives a separable equation whose integral is the arctangent; applying the first condition fixes c=0c=0, and integrating tanx\tan x gives lncosx-\ln|\cos x|. Independent check by differentiation: y=ln(cosx)y=-\ln(\cos x) gives y=tanxy'=\tan x and y=sec2x=1+tan2x=1+(y)2y''=\sec^2x=1+\tan^2x=1+\left(y'\right)^2.
5
  • The equation becomes d2ydu24dydu+4y=e2u\dfrac{\mathrm{d}^{2}y}{\mathrm{d}u^{2}}-4\dfrac{\mathrm{d}y}{\mathrm{d}u}+4y=\mathrm{e}^{2u}
  • The auxiliary equation m24m+4=0m^{2}-4m+4=0 has the repeated root m=2m=2, so the complementary function is (A+Bu)e2u(A+Bu)\mathrm{e}^{2u}
  • Because 22 is a repeated root, try y=Cu2e2uy=Cu^{2}\mathrm{e}^{2u}, giving 2Ce2u=e2u2C\mathrm{e}^{2u}=\mathrm{e}^{2u} and C=12C=\dfrac12
  • y=(A+Bu+u22)e2uy=\left(A+Bu+\dfrac{u^{2}}{2}\right)\mathrm{e}^{2u}
  • y=x2(A+Blnx+(lnx)22)y=x^{2}\left(A+B\ln x+\dfrac{(\ln x)^{2}}{2}\right)
8
(8 marks)8
Notes
Using xdydx=yux\tfrac{\mathrm{d}y}{\mathrm{d}x}=y_u and x2d2ydx2=yuuyux^2\tfrac{\mathrm{d}^2y}{\mathrm{d}x^2}=y_{uu}-y_u turns the left side into yuu4yu+4yy_{uu}-4y_u+4y, while x2=e2ux^2=\mathrm{e}^{2u}. The repeated root forces a u2u^2 factor in the particular integral. Independent check by substitution: for y=12x2(lnx)2y=\tfrac12x^2(\ln x)^2, y=xlnx+x(lnx)2y'=x\ln x+x(\ln x)^2 and y=1+3lnx+(lnx)2y''=1+3\ln x+(\ln x)^2, so x2y3xy+4y=x2[1+3lnx+(lnx)23lnx3(lnx)2+2(lnx)2]=x2x^2y''-3xy'+4y=x^2\left[1+3\ln x+(\ln x)^2-3\ln x-3(\ln x)^2+2(\ln x)^2\right]=x^2.