Method of variation of parameters

At a Glance

Why This Chapter Matters

Variation of parameters appears in 12 of the last 14 years — only two years missed, making it the most consistently examined technique in Paper 1 Section B. The method works on any second-order linear ODE regardless of the right-hand side: it handles sec⁡\sec, log⁡\log, tan⁡\tan, polynomials, and combinations that undetermined coefficients cannot touch. In every question the four-step skeleton is the same; the skill is recognising which variant you need (standard CF, Cauchy-Euler, or reduction-of-order) before the VoP machinery kicks in.

Minimum Theory

The formula. Given y′′+P(x)y′+Q(x)y=g(x)y''+P(x)y'+Q(x)y=g(x) with two complementary functions y1,y2y_1,y_2, seek yp=u1y1+u2y2y_p=u_1y_1+u_2y_2 where u1′=−y2 gW,u2′=y1 gW,W=y1y2′−y2y1′.u_1'=-\frac{y_2\,g}{W},\qquad u_2'=\frac{y_1\,g}{W},\qquad W=y_1y_2'-y_2y_1'. This is the standard form — the ODE must have leading coefficient 11 before you read off g(x)g(x). For ay′′+…=R(x)ay''+\ldots=R(x), divide everything by aa first; then g=R/ag=R/a.

Two constraints, two equations. The conditions u1′y1+u2′y2=0u_1'y_1+u_2'y_2=0 and u1′y1′+u2′y2′=gu_1'y_1'+u_2'y_2'=g uniquely determine u1′u_1' and u2′u_2' via Cramer’s rule — the formulas above.

Getting both CF solutions. The VoP formula needs two independent homogeneous solutions. Three sub-cases arise:

  1. Constant coefficients (most common): solve the auxiliary equation; the roots give exponential, trigonometric, or repeated-root CF.
  2. Cauchy-Euler (x2y′′−…x^2y''-\ldots): try y=xmy=x^m to get the indicial equation; roots m1,m2m_1,m_2 give y1=xm1y_1=x^{m_1}, y2=xm2y_2=x^{m_2}.
  3. One CF given: use reduction of order (y2=v(x)y1y_2=v(x)y_1) or operator factorisation to find the second.

Question Archetypes

Three patterns cover all VoP questions.

ArchetypeYou are seeing this when…
variation-of-parametersa standard constant-coefficient ODE with an “awkward” RHS
vop-cauchy-eulerthe equation has x2y′′, xy′x^2y'',\,xy' terms (Euler–Cauchy type)
vop-after-reductionone CF solution is given and you must find the second

variation-of-parameters (5 question(s); 2013, 2014, 2016, 2017, 2018)

Recognition Cues

Solution Template

  1. Write the auxiliary equation and find the two CF solutions y1,y2y_1,y_2.
  2. Compute W=y1y2′−y2y1′W=y_1y_2'-y_2y_1'.
  3. Write u1′=−y2g/Wu_1'=-y_2g/W and u2′=y1g/Wu_2'=y_1g/W where gg is the RHS of the standard-form ODE.
  4. Integrate to find u1,u2u_1,u_2. Use standard integrals: ∫tan⁡(ax) dx=−1aln⁡∣cos⁡(ax)∣\int\tan(ax)\,dx=-\tfrac1a\ln|\cos(ax)|; ∫sec⁡(2x) dx=12ln⁡∣sec⁡2x+tan⁡2x∣\int\sec(2x)\,dx=\tfrac12\ln|\sec2x+\tan2x|; ∫eaxsin⁡(bx) dx=eax(asin⁡bx−bcos⁡bx)a2+b2\int e^{ax}\sin(bx)\,dx=\tfrac{e^{ax}(a\sin bx-b\cos bx)}{a^2+b^2}; ∫xlog⁡x dx=x22log⁡x−x24\int x\log x\,dx=\tfrac{x^2}{2}\log x-\tfrac{x^2}{4}.
  5. Write yp=u1y1+u2y2y_p=u_1y_1+u_2y_2 and simplify using trig identities if needed.
  6. General solution: y=yc+ypy=y_c+y_p.

Worked Example(s)

2013 Paper 1, 2013-P1-Q6b (10 marks)

Solve y′′+a2y=sec⁡axy''+a^2y=\sec ax by variation of parameters.

CF. Auxiliary equation r2+a2=0⇒y1=cos⁡ax, y2=sin⁡axr^2+a^2=0\Rightarrow y_1=\cos ax,\,y_2=\sin ax.

Wronskian. W=acos⁡2ax+asin⁡2ax=aW=a\cos^2ax+a\sin^2ax=a.

Integrands (g=sec⁡axg=\sec ax): u1′=−sin⁡ax⋅sec⁡axa=−tan⁡axa  ⇒  u1=ln⁡∣cos⁡ax∣a2.u_1'=-\frac{\sin ax\cdot\sec ax}{a}=-\frac{\tan ax}{a}\;\Rightarrow\;u_1=\frac{\ln|\cos ax|}{a^2}. u2′=cos⁡ax⋅sec⁡axa=1a  ⇒  u2=xa.u_2'=\frac{\cos ax\cdot\sec ax}{a}=\frac{1}{a}\;\Rightarrow\;u_2=\frac{x}{a}.

Particular integral: yp=cos⁡axa2ln⁡∣cos⁡ax∣+xsin⁡axa.y_p=\frac{\cos ax}{a^2}\ln|\cos ax|+\frac{x\sin ax}{a}.

  y=C1cos⁡ax+C2sin⁡ax+cos⁡axa2ln⁡∣cos⁡ax∣+xsin⁡axa.  \boxed{\;y=C_1\cos ax+C_2\sin ax+\frac{\cos ax}{a^2}\ln|\cos ax|+\frac{x\sin ax}{a}.\;}


2016 Paper 1, 2016-P1-Q6b (15 marks)

Solve (D2+2D+1)y=e−xlog⁡x(D^2+2D+1)y=e^{-x}\log x by variation of parameters.

CF. (D+1)2=0(D+1)^2=0 — repeated root D=−1D=-1: y1=e−xy_1=e^{-x}, y2=xe−xy_2=xe^{-x}.

Wronskian. W=e−2xW=e^{-2x}.

Integrands (g=e−xlog⁡xg=e^{-x}\log x): the exponentials cancel: y2g/W=xlog⁡xy_2g/W=x\log x and y1g/W=log⁡xy_1g/W=\log x.

∫xlog⁡x dx=x22log⁡x−x24,∫log⁡x dx=xlog⁡x−x.\int x\log x\,dx=\tfrac{x^2}{2}\log x-\tfrac{x^2}{4},\qquad\int\log x\,dx=x\log x-x.

Assemble: yp=−e−x ⁣(x22log⁡x−x24)+xe−x(xlog⁡x−x)=e−x ⁣(x22log⁡x−3x24).y_p=-e^{-x}\!\left(\tfrac{x^2}{2}\log x-\tfrac{x^2}{4}\right)+xe^{-x}(x\log x-x)=e^{-x}\!\left(\tfrac{x^2}{2}\log x-\tfrac{3x^2}{4}\right).

  y=(c1+c2x)e−x+e−x ⁣(x22log⁡x−3x24).  \boxed{\;y=(c_1+c_2x)e^{-x}+e^{-x}\!\left(\frac{x^2}{2}\log x-\frac{3x^2}{4}\right).\;}


2018 Paper 1, 2018-P1-Q6c (13 marks)

Solve y′′+16y=32sec⁡2xy''+16y=32\sec2x.

CF. r2+16=0⇒y1=cos⁡4x, y2=sin⁡4xr^2+16=0\Rightarrow y_1=\cos4x,\,y_2=\sin4x; W=4W=4.

Compute u1,u2u_1,u_2 (g=32sec⁡2xg=32\sec2x): u1′=−sin⁡4x⋅32sec⁡2x4=−8⋅sin⁡4xcos⁡2x.u_1'=-\frac{\sin4x\cdot32\sec2x}{4}=-8\cdot\frac{\sin4x}{\cos2x}. Use sin⁡4x=2sin⁡2xcos⁡2x\sin4x=2\sin2x\cos2x: u1′=−16sin⁡2x⇒u1=8cos⁡2xu_1'=-16\sin2x\Rightarrow u_1=8\cos2x.

u2′=cos⁡4x⋅32sec⁡2x4=8⋅cos⁡4xcos⁡2x.u_2'=\frac{\cos4x\cdot32\sec2x}{4}=8\cdot\frac{\cos4x}{\cos2x}. Use cos⁡4x=2cos⁡22x−1\cos4x=2\cos^22x-1: u2′=16cos⁡2x−8sec⁡2x⇒u2=8sin⁡2x−4ln⁡∣sec⁡2x+tan⁡2x∣u_2'=16\cos2x-8\sec2x\Rightarrow u_2=8\sin2x-4\ln|\sec2x+\tan2x|.

Combine: u1y1+u2y2u_1y_1+u_2y_2 has elementary part 8(cos⁡2xcos⁡4x+sin⁡2xsin⁡4x)=8cos⁡2x8(\cos2x\cos4x+\sin2x\sin4x)=8\cos2x: yp=8cos⁡2x−4sin⁡4xln⁡∣sec⁡2x+tan⁡2x∣.y_p=8\cos2x-4\sin4x\ln|\sec2x+\tan2x|.

  y=C1cos⁡4x+C2sin⁡4x+8cos⁡2x−4sin⁡4xln⁡∣sec⁡2x+tan⁡2x∣.  \boxed{\;y=C_1\cos4x+C_2\sin4x+8\cos2x-4\sin4x\ln|\sec2x+\tan2x|.\;}


2014 Paper 1, 2014-P1-Q6a (10 marks)

Solve y′−5y=sin⁡xy'-5y=\sin x by variation of parameters.

First-order case. CF: y1=e5xy_1=e^{5x}. Try yp=u(x)e5xy_p=u(x)e^{5x}; substituting: u′e5x=sin⁡x⇒u′=e−5xsin⁡xu'e^{5x}=\sin x\Rightarrow u'=e^{-5x}\sin x.

Using ∫eaxsin⁡bx=eax(asin⁡bx−bcos⁡bx)a2+b2\int e^{ax}\sin bx=\tfrac{e^{ax}(a\sin bx-b\cos bx)}{a^2+b^2} with a=−5,b=1a=-5,b=1: u=−e−5x(5sin⁡x+cos⁡x)26  ⇒  yp=−5sin⁡x+cos⁡x26.u=-\frac{e^{-5x}(5\sin x+\cos x)}{26}\;\Rightarrow\;y_p=-\frac{5\sin x+\cos x}{26}.

  y=Ce5x−5sin⁡x+cos⁡x26.  \boxed{\;y=Ce^{5x}-\frac{5\sin x+\cos x}{26}.\;}


2017 Paper 1, 2017-P1-Q7b-ii (8 marks)

Solve y′′−y′−2y=44−76x−48x2y''-y'-2y=44-76x-48x^2 by variation of parameters.

CF. m2−m−2=0⇒m=2,−1m^2-m-2=0\Rightarrow m=2,-1; y1=e−xy_1=e^{-x}, y2=e2xy_2=e^{2x}; W=3exW=3e^x.

Using ∫exP dx=ex(P−P′+P′′−⋯ )\int e^x P\,dx=e^x(P-P'+P''-\cdots) with P=44−76x−48x2P=44-76x-48x^2: u1y1+u2y2=24x2+14x−5(exponential factors cancel).u_1y_1+u_2y_2=24x^2+14x-5\qquad(\text{exponential factors cancel}).

  y=C1e−x+C2e2x+24x2+14x−5.  \boxed{\;y=C_1e^{-x}+C_2e^{2x}+24x^2+14x-5.\;}

Common Traps


vop-cauchy-euler (2 question(s); 2019, 2024)

Recognition Cues

Solution Template

  1. Solve the homogeneous Cauchy-Euler ODE by trying y=xmy=x^m; get the indicial equation.
  2. Write down y1=xm1y_1=x^{m_1} and y2=xm2y_2=x^{m_2}.
  3. Divide the full ODE by x2x^2 to get standard form; read off g(x)g(x) from the normalised RHS.
  4. Compute W=y1y2′−y2y1′W=y_1y_2'-y_2y_1'.
  5. Apply VoP: u1′=−y2g/Wu_1'=-y_2g/W, u2′=y1g/Wu_2'=y_1g/W; integrate; assemble ypy_p.

Worked Example(s)

2019 Paper 1, 2019-P1-Q7a (15 marks) and 2024 Paper 1, 2024-P1-Q6c-ii (10 marks)

Find the independent CF solutions of x2y′′−2xy′+2y=x3sin⁡xx^2y''-2xy'+2y=x^3\sin x and find the general solution by variation of parameters.

Sources:,

Indicial equation. Try y=xmy=x^m in x2y′′−2xy′+2y=0x^2y''-2xy'+2y=0: m(m−1)−2m+2=m2−3m+2=(m−1)(m−2)=0m(m-1)-2m+2=m^2-3m+2=(m-1)(m-2)=0, giving y1=x,y2=x2.y_1=x,\qquad y_2=x^2.

Standard form. Divide by x2x^2: y′′−(2/x)y′+(2/x2)y=xsin⁡xy''-(2/x)y'+(2/x^2)y=x\sin x, so g(x)=xsin⁡xg(x)=x\sin x.

Wronskian. W=x⋅2x−x2⋅1=x2W=x\cdot2x-x^2\cdot1=x^2.

VoP integrals: u1′=−x2⋅xsin⁡xx2=−xsin⁡x  ⇒  u1=xcos⁡x−sin⁡x.u_1'=-\frac{x^2\cdot x\sin x}{x^2}=-x\sin x\;\Rightarrow\;u_1=x\cos x-\sin x. u2′=x⋅xsin⁡xx2=sin⁡x  ⇒  u2=−cos⁡x.u_2'=\frac{x\cdot x\sin x}{x^2}=\sin x\;\Rightarrow\;u_2=-\cos x.

Particular integral: yp=(xcos⁡x−sin⁡x)⋅x+(−cos⁡x)⋅x2=x2cos⁡x−xsin⁡x−x2cos⁡x=−xsin⁡x.y_p=(x\cos x-\sin x)\cdot x+(-\cos x)\cdot x^2=x^2\cos x-x\sin x-x^2\cos x=-x\sin x.

  y=C1x+C2x2−xsin⁡x.  \boxed{\;y=C_1x+C_2x^2-x\sin x.\;}

Common Traps


vop-after-reduction (4 question(s); 2020, 2021, 2022, 2025)

Recognition Cues

Solution Template

  1. Accept the given y1y_1 (or find it by inspection/trial).
  2. Reduction of order: substitute y2=v(x)y1y_2=v(x)y_1 into the homogeneous ODE; reduce to a first-order ODE in u=v′u=v'; integrate twice to get vv and hence y2y_2.
  3. Divide the full ODE by its leading coefficient to get standard form; read off g(x)g(x).
  4. Compute W=y1y2′−y2y1′W=y_1y_2'-y_2y_1'.
  5. Apply VoP: u1′=−y2g/Wu_1'=-y_2g/W, u2′=y1g/Wu_2'=y_1g/W; integrate; assemble ypy_p.

Worked Example(s)

2021 Paper 1, 2021-P1-Q8a-ii (10 marks)

Solve x2y′′−2x(1+x)y′+2(1+x)y=x3x^2y''-2x(1+x)y'+2(1+x)y=x^3 by variation of parameters, given y1=xy_1=x satisfies the homogeneous equation.

Find y2y_2. Try y2=v(x)⋅xy_2=v(x)\cdot x. Substituting into the homogeneous ODE and simplifying: x3v′′−2x3v′=0  ⇒  v′′=2v′  ⇒  u=v′=e2x  ⇒  v=e2x/2.x^3v''-2x^3v'=0\;\Rightarrow\;v''=2v'\;\Rightarrow\;u=v'=e^{2x}\;\Rightarrow\;v=e^{2x}/2. Take y2=xe2xy_2=xe^{2x}.

Standard form. Divide by x2x^2: g(x)=x3/x2=xg(x)=x^3/x^2=x.

Wronskian. W=x⋅(1+2x)e2x−xe2x⋅1=2x2e2xW=x\cdot(1+2x)e^{2x}-xe^{2x}\cdot1=2x^2e^{2x}.

VoP: u2′=x⋅x2x2e2x=12e−2x⇒u2=−14e−2xu_2'=\tfrac{x\cdot x}{2x^2e^{2x}}=\tfrac12e^{-2x}\Rightarrow u_2=-\tfrac14e^{-2x}. Then u1′=−12⇒u1=−x/2u_1'=-\tfrac12\Rightarrow u_1=-x/2.

yp=(−x/2)(x)+(−e−2x/4)(xe2x)=−x2/2−x/4.y_p=(-x/2)(x)+(-e^{-2x}/4)(xe^{2x})=-x^2/2-x/4.

The −x/4-x/4 is absorbed into C1xC_1x:

  y=C1x+C2xe2x−x22.  \boxed{\;y=C_1x+C_2xe^{2x}-\frac{x^2}{2}.\;}


2022 Paper 1, 2022-P1-Q6b (15 marks)

Solve (x2−1)y′′−2xy′+2y=(x2−1)2(x^2-1)y''-2xy'+2y=(x^2-1)^2 by variation of parameters, given y1=xy_1=x.

Find y2y_2. Try y2=vxy_2=vx; substituting into the homogeneous equation: x(x2−1)v′′−2v′=0  ⇒  dv′v′=2 dxx(x2−1).x(x^2-1)v''-2v'=0\;\Rightarrow\;\frac{dv'}{v'}=\frac{2\,dx}{x(x^2-1)}. Partial fractions: 2x(x−1)(x+1)=−2x+1x−1+1x+1\tfrac{2}{x(x-1)(x+1)}=-\tfrac2x+\tfrac1{x-1}+\tfrac1{x+1}. Integrating: v′=(x2−1)/x2=1−1/x2v'=(x^2-1)/x^2=1-1/x^2, so v=x+1/xv=x+1/x and y2=x2+1y_2=x^2+1.

Standard form. Divide by (x2−1)(x^2-1): g=x2−1g=x^2-1.

Wronskian. W=x⋅2x−(x2+1)⋅1=x2−1W=x\cdot2x-(x^2+1)\cdot1=x^2-1.

VoP: u2′=x⇒u2=x2/2u_2'=x\Rightarrow u_2=x^2/2; u1′=−(x2+1)⇒u1=−x3/3−xu_1'=-(x^2+1)\Rightarrow u_1=-x^3/3-x.

yp=(−x3/3−x)⋅x+(x2/2)⋅(x2+1)=x46−x22.y_p=(-x^3/3-x)\cdot x+(x^2/2)\cdot(x^2+1)=\frac{x^4}{6}-\frac{x^2}{2}.

  y=C1x+C2(x2+1)+x46−x22.  \boxed{\;y=C_1x+C_2(x^2+1)+\frac{x^4}{6}-\frac{x^2}{2}.\;}


2020 Paper 1, 2020-P1-Q6a (20 marks)

Solve y′′+(1−cot⁡x)y′−ycot⁡x=sin⁡2xy''+(1-\cot x)y'-y\cot x=\sin^2 x by variation of parameters, given y1=e−xy_1=e^{-x}.

Find y2y_2. Factor the operator: (D−cot⁡x)(D+1)y=0(D-\cot x)(D+1)y=0. Letting v=(D+1)yv=(D+1)y: (D−cot⁡x)v=0⇒v=sin⁡x(D-\cot x)v=0\Rightarrow v=\sin x. Solve (D+1)y=sin⁡x(D+1)y=\sin x: integrating factor exe^x: y2=sin⁡x−cos⁡xy_2=\sin x-\cos x.

Wronskian. W=2e−xsin⁡xW=2e^{-x}\sin x.

VoP: u2′=e−xsin⁡2x2e−xsin⁡x=sin⁡x2  ⇒  u2=−cos⁡x2.u_2'=\frac{e^{-x}\sin^2 x}{2e^{-x}\sin x}=\frac{\sin x}{2}\;\Rightarrow\;u_2=-\frac{\cos x}{2}. u1′=−(sin⁡x−cos⁡x)sin⁡2x2e−xsin⁡x=−ex4(1−cos⁡2x−sin⁡2x)  ⇒  u1=ex20(3sin⁡2x−cos⁡2x−5).u_1'=-\frac{(\sin x-\cos x)\sin^2 x}{2e^{-x}\sin x}=-\frac{e^x}{4}(1-\cos2x-\sin2x)\;\Rightarrow\;u_1=\frac{e^x}{20}(3\sin2x-\cos2x-5).

Assembling and simplifying (constant terms cancel): yp=−110sin⁡2x+15cos⁡2x.y_p=-\frac{1}{10}\sin2x+\frac{1}{5}\cos2x.

  y=C1e−x+C2(sin⁡x−cos⁡x)−sin⁡2x10+cos⁡2x5.  \boxed{\;y=C_1e^{-x}+C_2(\sin x-\cos x)-\frac{\sin2x}{10}+\frac{\cos2x}{5}.\;}


2025 Paper 1, 2025-P1-Q8a (15 marks)

Solve (x+2)y′′−(2x+5)y′+2y=(1+x)ex(x+2)y''-(2x+5)y'+2y=(1+x)e^x by variation of parameters.

CF by inspection. Try y=emxy=e^{mx}: matching coefficients of xx gives m=2m=2, yielding y1=e2xy_1=e^{2x}. Try y=αx+βy=\alpha x+\beta: gives y2=2x+5y_2=2x+5.

Standard form. Divide by (x+2)(x+2): g=(1+x)ex/(x+2)g=(1+x)e^x/(x+2).

Wronskian. W=−4(x+2)e2xW=-4(x+2)e^{2x}.

VoP: u2′=−(x+1)ex4(x+2)2u_2'=-\tfrac{(x+1)e^x}{4(x+2)^2}; use ddx ⁣exx+2=(x+1)ex(x+2)2\tfrac{d}{dx}\!\tfrac{e^x}{x+2}=\tfrac{(x+1)e^x}{(x+2)^2}, so u2=−ex4(x+2)u_2=-\tfrac{e^x}{4(x+2)}.

After assembling, both terms combine to give yp=−exy_p=-e^x.

  y=C1e2x+C2(2x+5)−ex.  \boxed{\;y=C_1e^{2x}+C_2(2x+5)-e^x.\;}

Common Traps


Marks-Aware Writing

8-mark questions (2017): CF + Wronskian (one line each), two VoP integrals (show clearly), assemble and simplify. Since forcing is polynomial, the exponentials in u1y1+u2y2u_1y_1+u_2y_2 cancel — state this explicitly.

10-mark questions (2013, 2014, 2024): Write CF and Wronskian; show both integrands; integrate; write ypy_p neatly; state the general solution. Four to five working lines suffice.

13-15-mark questions (2016, 2018, 2019, 2022, 2025): Full layout — CF with justification, Wronskian calculation (show the 2×22\times2 determinant), both integrands and their integrals step by step, assembled ypy_p, boxed final answer.

20-mark questions (2020): All of the above, plus the derivation of y2y_2 (operator factorisation or reduction of order written out in full), Wronskian computation, all four integrals shown. Double-check the constant cancellations.

Practice Set

YearPaper/QMarksArchetypeOne-line hint
2025P1-Q8a15vop-after-reductionCF: e2xe^{2x} and 2x+52x+5 by inspection; W=−4(x+2)e2xW=-4(x+2)e^{2x}; yp=−exy_p=-e^x telescopes neatly
2024P1-Q6c-ii10vop-cauchy-eulerSame as 2019; indicial roots 1,2; g=xsin⁡xg=x\sin x; yp=−xsin⁡xy_p=-x\sin x
2022P1-Q6b15vop-after-reductionPartial fractions to find v′=(x2−1)/x2v'=(x^2-1)/x^2; y2=x2+1y_2=x^2+1; yp=x4/6−x2/2y_p=x^4/6-x^2/2
2021P1-Q8a-ii10vop-after-reductiony2=xe2xy_2=xe^{2x} from v′′=2v′v''=2v'; standard form g=xg=x; yp=−x2/2y_p=-x^2/2
2020P1-Q6a20vop-after-reductionOperator factor (D−cot⁡x)(D+1)(D-\cot x)(D+1); y2=sin⁡x−cos⁡xy_2=\sin x-\cos x; yp=−110sin⁡2x+15cos⁡2xy_p=-\tfrac{1}{10}\sin2x+\tfrac15\cos2x
2019P1-Q7a15vop-cauchy-eulerIndicial roots 1,2; g=xsin⁡xg=x\sin x after dividing by x2x^2; yp=−xsin⁡xy_p=-x\sin x
2018P1-Q6c13variation-of-parametersW=4W=4; double-angle identities; $y_p=8\cos2x-4\sin4x\ln
2017P1-Q7b-ii8variation-of-parametersW=3exW=3e^x; ∫exP dx\int e^xP\,dx shortcut; exponentials cancel; yp=24x2+14x−5y_p=24x^2+14x-5
2016P1-Q6b15variation-of-parametersRepeated root; W=e−2xW=e^{-2x}; ∫xlog⁡x\int x\log x and ∫log⁡x\int\log x; yp=e−x(x22log⁡x−3x24)y_p=e^{-x}(\tfrac{x^2}{2}\log x-\tfrac{3x^2}{4})
2014P1-Q6a10variation-of-parametersFirst-order VoP; ∫e−5xsin⁡x dx\int e^{-5x}\sin x\,dx; denominator 26; yp=−(5sin⁡x+cos⁡x)/26y_p=-(5\sin x+\cos x)/26
2013P1-Q6b10variation-of-parametersW=aW=a; $\int\tan ax=-\tfrac{1}{a}\ln

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