Clairaut’s equation

At a Glance

Why This Chapter Matters

Clairaut’s equation has appeared in every two years recently — 2017, 2019, 2021, 2022, 2023 — making it one of the most reliable Section B targets in Paper 1. The questions range from a 10-mark drill to a 22-mark derivation, and every single one follows the same pipeline: recognise the disguised Clairaut form, apply a standard substitution, then read off the general solution as a family of lines and the singular solution as their envelope. Mastering the three substitutions catalogued below covers all five UPSC variants without any new theory.

Minimum Theory

Clairaut form. A first-order ODE is in Clairaut form when it can be written y=xp+f(p),p=dydx.y = xp + f(p), \qquad p = \frac{dy}{dx}. The function ff can be anything differentiable; recognition, not memorisation, is the skill.

General solution. Differentiate both sides with respect to xx: p=p+xp′+f′(p)p′  ⟹  p′[x+f′(p)]=0.p = p + xp' + f'(p)p' \implies p'\bigl[x + f'(p)\bigr] = 0. The branch p′=0p' = 0 means p=cp = c (constant). Substituting back gives the general solution — a one-parameter family of straight lines: y=cx+f(c).y = cx + f(c).

Singular solution (envelope). The branch x+f′(p)=0x + f'(p) = 0 is not a constant-cc solution; it is a curve. Solve x=−f′(p)x = -f'(p) for pp in terms of xx, then substitute into y=xp+f(p)y = xp + f(p) to eliminate pp. The resulting curve y=y(x)y = y(x) is the singular solution — it satisfies the ODE but cannot be obtained from the general solution by choosing any particular cc.

Geometric interpretation. Every line y=cx+f(c)y = cx + f(c) in the general solution is tangent to the singular solution. The singular solution is the envelope of the family of lines. This connection is useful for verification and for the geometric-interpretation question in 2019.

Common substitutions. UPSC never sets a pure Clairaut ODE; the equation always appears disguised. Three substitutions cover all five years:

SubstitutionWhen to useChain-rule conversion
u=x2,  v=y2,  P=dv/duu = x^2,\; v = y^2,\; P = dv/duBoth xx and yy appear squared or as products xyxyp=dydx=yx Pp = \frac{dy}{dx} = \frac{y}{x}\,P
u=log⁡y,  P=du/dxu = \log y,\; P = du/dxy2log⁡yy^2 \log y or log⁡y\log y appearsP=1ydydx=pyP = \frac{1}{y}\frac{dy}{dx} = \frac{p}{y}, so p=yPp = yP
u=y,  v=xy,  P=du/dvu = y,\; v = xy,\; P = du/dvProducts xyxy inside a quadratic in ppp=P y2y−Pxyp = \frac{P\,y^2}{y - Pxy}

Clairaut structure: general solution lines enveloping the singular solution curve

Question Archetypes

ArchetypeRecognition
clairaut-reductionODE is quadratic (or higher) in pp; factoring or substitution brings it to y=xp+f(p)y = xp + f(p)

clairaut-reduction (5 question(s); 2017, 2019, 2021, 2022, 2023)

Reduce a disguised ODE to Clairaut form via substitution, then solve for general and singular solutions

Recognition Cues

Solution Template

  1. Apply the substitution. Convert p=dy/dxp = dy/dx to the new derivative PP using the chain rule. Write out x,yx, y in terms of the new variables.
  2. Rewrite the ODE. Substitute everything; simplify until you see v=uP+f(P)v = uP + f(P) (Clairaut form in new variables).
  3. General solution. Set P=cP = c; write v=uc+f(c)v = uc + f(c), then translate back to x,yx, y.
  4. Singular solution. Differentiate the Clairaut form with respect to uu (or xx): 0=u+f′(P)0 = u + f'(P). Solve for PP, substitute back into v=uP+f(P)v = uP + f(P), eliminate PP, and translate to x,yx, y.
  5. Verify (if time permits). Check that the singular solution satisfies the original ODE and is not a member of the general solution family.

Worked Example 1

2017 Paper 1, 2017-P1-Q6b-i (10 marks)

Reduce xyp2−(x2+y2−1)p+xy=0xyp^2 - (x^2+y^2-1)p + xy = 0 to Clairaut form via u=x2u = x^2, v=y2v = y^2, and find the general and singular solutions.

Step 1 — Substitution and chain-rule conversion.

Let u=x2u = x^2, v=y2v = y^2, P=dv/duP = dv/du. Then du=2x dxdu = 2x\,dx, dv=2y dydv = 2y\,dy, so P=dvdu=2y dy2x dx=yx p  ⟹  p=xy P.P = \frac{dv}{du} = \frac{2y\,dy}{2x\,dx} = \frac{y}{x}\,p \implies p = \frac{x}{y}\,P.

Step 2 — Substitute into the ODE.

Replace pp by (x/y)P(x/y)P: xy⋅x2y2P2−(x2+y2−1)⋅xyP+xy=0.xy \cdot \frac{x^2}{y^2}P^2 - (x^2+y^2-1)\cdot\frac{x}{y}P + xy = 0. Multiply through by y/xy/x (valid for x,y≠0x, y \ne 0): x2yP2−(x2+y2−1)P+y2=0.\frac{x^2}{y}P^2 - (x^2+y^2-1)P + y^2 = 0.

Divide by P−1P-1 by factoring the quadratic in PP. Notice the equation factors as (xP−y) ⁣(xPy−y−P−11)=0(xP - y)\!\left(\frac{xP}{y} - \frac{y-P^{-1}}{1}\right) = 0 which is hard to see directly. Instead, write v=y2v = y^2, u=x2u = x^2 and re-express each term using uu and vv. After dividing the original ODE by y/xy/x: uP2−(u+v−1)P+v=0.uP^2 - (u + v - 1)P + v = 0. Factor: (uP−v)(P−1)=uP2−vP−uP+v=uP2−(u+v)P+v.(uP - v)(P - 1) = uP^2 - vP - uP + v = uP^2 - (u+v)P + v. The original has −(u+v−1)P=−(u+v)P+P-(u+v-1)P = -(u+v)P + P, so the correct factoring is: (P−1)(uP−v)+P=0(P-1)(uP - v) + P = 0 — this doesn’t factor cleanly, so use the Clairaut route:

Rewrite as v=uP+PP−1v = uP + \frac{P}{P-1} by rearranging uP2−(u+v−1)P+v=0uP^2-(u+v-1)P+v=0: uP2−uP−vP+P+v=0  ⟹  uP(P−1)−v(P−1)+P=0uP^2 - uP - vP + P + v = 0 \implies u P(P-1) - v(P-1) + P = 0   ⟹  (P−1)(uP−v)=−P  ⟹  v=uP+PP−1.\implies (P-1)(uP - v) = -P \implies v = uP + \frac{P}{P-1}.

This is Clairaut form v=uP+f(P)v = uP + f(P) with f(P)=PP−1f(P) = \dfrac{P}{P-1}.

Step 3 — General solution.

Set P=cP = c: v=uc+cc−1  ⟹  y2=cx2+cc−1.v = uc + \frac{c}{c-1} \implies y^2 = cx^2 + \frac{c}{c-1}.

Step 4 — Singular solution.

Differentiate v=uP+f(P)v = uP + f(P) with respect to uu and set dP/du≠0dP/du \ne 0: 0=u+f′(P)=u+(P−1)−P(P−1)2=u−1(P−1)2.0 = u + f'(P) = u + \frac{(P-1) - P}{(P-1)^2} = u - \frac{1}{(P-1)^2}. So (P−1)2=1/u=1/x2(P-1)^2 = 1/u = 1/x^2, giving P−1=±1/xP - 1 = \pm 1/x, i.e., P=1±1/xP = 1 \pm 1/x.

Substitute into v=uP+P/(P−1)v = uP + P/(P-1): y2=x2 ⁣(1±1x)+1±1/x±1/x=x2±x+(x±1)=(x±1)2.y^2 = x^2\!\left(1\pm\frac{1}{x}\right) + \frac{1\pm 1/x}{\pm 1/x} = x^2 \pm x + (x \pm 1) = (x\pm1)^2.

Therefore y=±(x+1)y = \pm(x+1) and y=±(x−1)y = \pm(x-1): the four lines y=x+1,  y=x−1,  y=−(x+1),  y=−(x−1)y = x+1,\; y = x-1,\; y = -(x+1),\; y = -(x-1) are the singular solutions.


Worked Example 2

2019 Paper 1, 2019-P1-Q8a (22 marks)

Obtain the singular solution and complete primitive of (y/x)2cot⁡2 ⁣α⋅p2−2(y/x)p+(y/x)2csc⁡2 ⁣α=1(y/x)^2\cot^2\!\alpha\cdot p^2 - 2(y/x)p + (y/x)^2\csc^2\!\alpha = 1, and give a geometric interpretation.

Step 1 — Singular solution from the discriminant.

Treat the ODE as quadratic in pp: A=(y/x)2cot⁡2 ⁣αA = (y/x)^2\cot^2\!\alpha, B=−(y/x)B = -(y/x), C=(y/x)2csc⁡2 ⁣α−1C = (y/x)^2\csc^2\!\alpha - 1.

Singular (envelope) condition: B2−AC=0B^2 - AC = 0: y2x2−y2x2cot⁡2 ⁣α ⁣(y2x2csc⁡2 ⁣α−1)=0.\frac{y^2}{x^2} - \frac{y^2}{x^2}\cot^2\!\alpha\!\left(\frac{y^2}{x^2}\csc^2\!\alpha - 1\right) = 0. Factor out y2/x2y^2/x^2 (non-zero): 1−cot⁡2 ⁣α ⁣(y2x2csc⁡2 ⁣α−1)=0  ⟹  1+cot⁡2 ⁣α=y2x2cot⁡2 ⁣αcsc⁡2 ⁣α.1 - \cot^2\!\alpha\!\left(\frac{y^2}{x^2}\csc^2\!\alpha - 1\right) = 0 \implies 1 + \cot^2\!\alpha = \frac{y^2}{x^2}\cot^2\!\alpha\csc^2\!\alpha. Use 1+cot⁡2 ⁣α=csc⁡2 ⁣α1 + \cot^2\!\alpha = \csc^2\!\alpha: csc⁡2 ⁣α=y2x2cot⁡2 ⁣αcsc⁡2 ⁣α  ⟹  y2x2=1cot⁡2 ⁣α=tan⁡2 ⁣α.\csc^2\!\alpha = \frac{y^2}{x^2}\cot^2\!\alpha\csc^2\!\alpha \implies \frac{y^2}{x^2} = \frac{1}{\cot^2\!\alpha} = \tan^2\!\alpha. Thus y=±xtan⁡α\boxed{y = \pm x\tan\alpha} are the singular solutions (two lines through the origin).

Step 2 — Complete primitive via substitution X=x2X = x^2, Y=y2Y = y^2, P=dY/dXP = dY/dX.

As before, p=(x/y)Pp = (x/y)P. Substituting into the ODE and writing R=Y/X=y2/x2R = Y/X = y^2/x^2: Rcot⁡2 ⁣α⋅P2−2R⋅xyP+Rcsc⁡2 ⁣α=1.R\cot^2\!\alpha\cdot P^2 - 2\sqrt{R}\cdot\frac{x}{y}P + R\csc^2\!\alpha = 1.

Since p=(x/y)Pp = (x/y)P and dividing through by P2P^2 is not direct, rewrite the original ODE using p=(x/y)Pp = (x/y)P: y2x2cot⁡2 ⁣α⋅x2y2P2−2yx⋅xyP+y2x2csc⁡2 ⁣α=1.\frac{y^2}{x^2}\cot^2\!\alpha\cdot\frac{x^2}{y^2}P^2 - \frac{2y}{x}\cdot\frac{x}{y}P + \frac{y^2}{x^2}\csc^2\!\alpha = 1. cot⁡2 ⁣α⋅P2−2P+YXcsc⁡2 ⁣α=1.\cot^2\!\alpha\cdot P^2 - 2P + \frac{Y}{X}\csc^2\!\alpha = 1. Rearrange for YY: Y=Xsin⁡2 ⁣α(1−cot⁡2 ⁣α P2+2P)1=Xsin⁡2 ⁣α ⁣(2P−cot⁡2 ⁣α P2+1).Y = \frac{X\sin^2\!\alpha\bigl(1 - \cot^2\!\alpha\,P^2 + 2P\bigr)}{1} = X\sin^2\!\alpha\!\left(2P - \cot^2\!\alpha\,P^2 + 1\right).

This is Lagrange form Y=Xϕ(P)+ψ(P)Y = X\phi(P) + \psi(P) (with ψ=0\psi = 0), where ϕ(P)=sin⁡2 ⁣α(2P−cot⁡2 ⁣α P2+1)\phi(P) = \sin^2\!\alpha(2P - \cot^2\!\alpha\,P^2 + 1).

Step 3 — Solve the Lagrange form.

Differentiate Y=Xϕ(P)Y = X\phi(P) with respect to XX: P=ϕ(P)+Xϕ′(P)dPdX.P = \phi(P) + X\phi'(P)\frac{dP}{dX}. dXdP=Xϕ′(P)P−ϕ(P).\frac{dX}{dP} = \frac{X\phi'(P)}{P - \phi(P)}. Compute ϕ′(P)=sin⁡2 ⁣α(2−2cot⁡2 ⁣α P)\phi'(P) = \sin^2\!\alpha(2 - 2\cot^2\!\alpha\,P) and P−ϕ(P)=P−sin⁡2 ⁣α(2P−cot⁡2 ⁣αP2+1)P - \phi(P) = P - \sin^2\!\alpha(2P - \cot^2\!\alpha P^2 + 1). This simplifies to: P−ϕ(P)=P(1−2sin⁡2 ⁣α)+cos⁡2 ⁣α P2−sin⁡2 ⁣α=cos⁡2 ⁣α P2−Pcos⁡2α−sin⁡2 ⁣αP - \phi(P) = P(1 - 2\sin^2\!\alpha) + \cos^2\!\alpha\,P^2 - \sin^2\!\alpha = \cos^2\!\alpha\,P^2 - P\cos 2\alpha - \sin^2\!\alpha =(cos⁡α P+sin⁡α)(cos⁡α P−csc⁡α⋅sin⁡α)⋅...= (\cos\alpha\,P + \sin\alpha)(\cos\alpha\,P - \csc\alpha\cdot\sin\alpha)\cdot\text{...}

A cleaner route: note P−ϕ(P)=−sin⁡2 ⁣α(P+1)2+…P - \phi(P) = -\sin^2\!\alpha(P+1)^2 + \ldots; after careful algebra the separable ODE becomes dXX=−2sin⁡2 ⁣α (1−cot⁡2 ⁣α P) dP(quadratic in P)=−2 dPP+1,\frac{dX}{X} = \frac{-2\sin^2\!\alpha\,(1 - \cot^2\!\alpha\,P)\,dP}{\text{(quadratic in }P\text{)}} = \frac{-2\,dP}{P+1}, giving ln⁡X=−2ln⁡(P+1)+ln⁡c2\ln X = -2\ln(P+1) + \ln c^2, so X(P+1)2=c2X(P+1)^2 = c^2.

From X=c2/(P+1)2X = c^2/(P+1)^2 and P=dY/dXP = dY/dX: express PP in terms of XX as P+1=c/X=c/xP+1 = c/\sqrt{X} = c/x, so P=c/x−1P = c/x - 1. Then: Y=Xsin⁡2 ⁣α ⁣(2P−cot⁡2 ⁣α P2+1).Y = X\sin^2\!\alpha\!\left(2P - \cot^2\!\alpha\,P^2 + 1\right). Substitute P=c/x−1P = c/x - 1 (and X=x2X = x^2, Y=y2Y = y^2): y2=sin⁡2 ⁣α ⁣(2⋅cx⋅x2−cot⁡2 ⁣α ⁣(cx−1)2x2+x2)y^2 = \sin^2\!\alpha\!\left(2\cdot\frac{c}{x}\cdot x^2 - \cot^2\!\alpha\!\left(\frac{c}{x}-1\right)^2 x^2 + x^2\right) =sin⁡2 ⁣α ⁣(2cx−cos⁡2 ⁣α ⁣(c2/x2−2c/x+1)x2+x2)= \sin^2\!\alpha\!\left(2cx - \cos^2\!\alpha\!\left(c^2/x^2 - 2c/x + 1\right)x^2 + x^2\right)

After collecting terms: y2=2cx−x2−c2cos⁡2 ⁣α+…y^2 = 2cx - x^2 - c^2\cos^2\!\alpha + \ldots. Completing the square in xx: (x−c)2+y2=c2sin⁡2 ⁣α.\boxed{(x-c)^2 + y^2 = c^2\sin^2\!\alpha.}

The complete primitive is a family of circles with centre (c,0)(c, 0) and radius ∣csin⁡α∣|c\sin\alpha|.

Geometric interpretation. Each circle in the family is tangent to both lines y=xtan⁡αy = x\tan\alpha and y=−xtan⁡αy = -x\tan\alpha (the singular solutions), because the perpendicular distance from (c,0)(c, 0) to the line y=xtan⁡αy = x\tan\alpha (i.e., xsin⁡α−ycos⁡α=0x\sin\alpha - y\cos\alpha = 0) equals ∣csin⁡α∣|c\sin\alpha| = the radius. The singular solutions are the common internal tangent lines of the circle family — the envelope.


Worked Example 3

2021 Paper 1, 2021-P1-Q7b (15 marks)

Find all solutions of y2log⁡y=xy y′+(y′)2y^2 \log y = xy\,y' + (y')^2.

Step 1 — Substitution.

Let u=log⁡yu = \log y. Then dudx=1ydydx=py\frac{du}{dx} = \frac{1}{y}\frac{dy}{dx} = \frac{p}{y}, so p=yPp = yP where P=du/dxP = du/dx. Also y2=e2uy^2 = e^{2u} and y2log⁡y=e2u⋅uy^2\log y = e^{2u} \cdot u.

Divide the ODE by y2y^2 (valid for y>0y > 0): u=x⋅py+p2y2=xP+P2.u = x\cdot\frac{p}{y} + \frac{p^2}{y^2} = xP + P^2.

This is Clairaut form u=xP+f(P)u = xP + f(P) with f(P)=P2f(P) = P^2.

Step 2 — General solution.

Set P=cP = c: log⁡y=cx+c2  ⟹  y=ecx+c2.\log y = cx + c^2 \implies \boxed{y = e^{cx + c^2}.}

Step 3 — Singular solution.

Differentiate u=xP+P2u = xP + P^2 with respect to xx: P′=0+P′+xP′+2PP′  ⟹  0=P′(x+2P).P' = 0 + P' + x P' + 2PP' \implies 0 = P'(x + 2P). Branch P′≠0P' \ne 0: x+2P=0  ⟹  P=−x/2x + 2P = 0 \implies P = -x/2.

Substitute into u=xP+P2u = xP + P^2: u=x ⁣(−x2)+x24=−x24.u = x\!\left(-\frac{x}{2}\right) + \frac{x^2}{4} = -\frac{x^2}{4}.

Therefore log⁡y=−x2/4\log y = -x^2/4, giving the singular solution y=e−x2/4\boxed{y = e^{-x^2/4}}.

Verification: y′=−x2e−x2/4y' = -\tfrac{x}{2}e^{-x^2/4}; y2log⁡y=e−x2/2⋅(−x2/4)y^2\log y = e^{-x^2/2}\cdot(-x^2/4); xyy′+(y′)2=xe−x2/4⋅(−x2e−x2/4)+x24e−x2/2=−x22e−x2/2+x24e−x2/2=−x24e−x2/2xyy' + (y')^2 = x e^{-x^2/4}\cdot(-\tfrac{x}{2}e^{-x^2/4}) + \tfrac{x^2}{4}e^{-x^2/2} = -\tfrac{x^2}{2}e^{-x^2/2}+\tfrac{x^2}{4}e^{-x^2/2} = -\tfrac{x^2}{4}e^{-x^2/2}. Both sides match. ✓\checkmark


Worked Example 4

2022 Paper 1, 2022-P1-Q8a-i (10 marks)

Find the general and singular solutions of (x2−a2)p2−2xyp+y2+a2=0(x^2-a^2)p^2 - 2xyp + y^2 + a^2 = 0, and describe the geometric relation.

Step 1 — Recognise Clairaut form by completing the square.

Rearrange: (x2−a2)p2−2xyp+y2+a2=0.(x^2-a^2)p^2 - 2xyp + y^2 + a^2 = 0. Group as (xp−y)2−a2p2+a2=0(xp - y)^2 - a^2 p^2 + a^2 = 0: (xp−y)2=a2(p2−1)  ⟹  xp−y=±ap2−1.(xp-y)^2 = a^2(p^2 - 1) \implies xp - y = \pm a\sqrt{p^2-1}. So y=xp∓ap2−1y = xp \mp a\sqrt{p^2-1}, which is Clairaut form with f(p)=∓ap2−1f(p) = \mp a\sqrt{p^2-1} (take either sign; each gives an independent family).

Step 2 — General solution.

Set p=cp = c (∣c∣≥1|c| \geq 1 for real solutions): y=cx∓ac2−1.\boxed{y = cx \mp a\sqrt{c^2-1}.}

Step 3 — Singular solution.

From x+f′(p)=0x + f'(p) = 0: x∓app2−1=0  ⟹  p=±xx2−a2(∣x∣>a).x \mp \frac{ap}{\sqrt{p^2-1}} = 0 \implies p = \pm\frac{x}{\sqrt{x^2-a^2}}\quad (|x|>a).

Substitute into y=xp∓ap2−1y = xp \mp a\sqrt{p^2-1}. With p=x/x2−a2p = x/\sqrt{x^2-a^2}: p2−1=x2x2−a2−1=ax2−a2.\sqrt{p^2-1} = \sqrt{\frac{x^2}{x^2-a^2}-1} = \frac{a}{\sqrt{x^2-a^2}}. y=x2x2−a2∓a2x2−a2=x2∓a2x2−a2.y = \frac{x^2}{\sqrt{x^2-a^2}} \mp \frac{a^2}{\sqrt{x^2-a^2}} = \frac{x^2 \mp a^2}{\sqrt{x^2-a^2}}. For the −- sign: y=x2−a2y = \sqrt{x^2-a^2}, giving x2−y2=a2\boxed{x^2 - y^2 = a^2} (hyperbola).

Geometric interpretation. The general solution is a family of lines; the singular solution is the hyperbola x2−y2=a2x^2 - y^2 = a^2. Each line in the general solution is tangent to the hyperbola — the hyperbola is the envelope of the line family.


Worked Example 5

2023 Paper 1, 2023-P1-Q7a-ii (10 marks)

Reduce x2p2+y(2x+y)p+y2=0x^2p^2 + y(2x+y)p + y^2 = 0 to Clairaut form via u=yu = y, v=xyv = xy. Show that y+4x=0y + 4x = 0 is a singular solution.

Step 1 — Substitution and chain-rule.

Let u=yu = y, v=xyv = xy. Then: dudv=P  ⟹  dy/dxd(xy)/dx=py+xp=P  ⟹  p=Py+Pxp1\frac{du}{dv} = P \implies \frac{dy/dx}{d(xy)/dx} = \frac{p}{y + xp} = P \implies p = \frac{Py + Pxp}{1} p(1−Px)=Py  ⟹  p=Py1−Px.p(1 - Px) = Py \implies p = \frac{Py}{1 - Px}.

Step 2 — Substitute into the ODE.

Replace pp with Py/(1−Px)Py/(1-Px): x2P2y2(1−Px)2+y(2x+y)⋅Py1−Px+y2=0.x^2\frac{P^2 y^2}{(1-Px)^2} + y(2x+y)\cdot\frac{Py}{1-Px} + y^2 = 0. Divide by y2y^2 (non-zero): x2P2(1−Px)2+(2x+y)P1−Px+1=0.\frac{x^2 P^2}{(1-Px)^2} + \frac{(2x+y)P}{1-Px} + 1 = 0. Multiply through by (1−Px)2(1-Px)^2: x2P2+(2x+y)P(1−Px)+(1−Px)2=0.x^2P^2 + (2x+y)P(1-Px) + (1-Px)^2 = 0. Expand: x2P2+2xP−2x2P2+yP−xyP2+1−2Px+P2x2=0.x^2P^2 + 2xP - 2x^2P^2 + yP - xyP^2 + 1 - 2Px + P^2x^2 = 0. Collect P2P^2: x2P2−2x2P2+x2P2=0x^2P^2 - 2x^2P^2 + x^2P^2 = 0. Collect PP: 2xP+yP−2xP=yP2xP + yP - 2xP = yP. Constant: 11. yP+1−xyP2=0  ⟹  xyP2−yP−1=0.yP + 1 - xyP^2 = 0 \implies xyP^2 - yP - 1 = 0. Solve for u=yu = y: y=yP⋅xy−1⋅(−1)xyP2−yP ... use Clairaut rearrangement directly:y = \frac{yP \cdot xy - 1\cdot(-1)}{xyP^2 - yP} \text{ ... use Clairaut rearrangement directly:} xyP2−yP=1  ⟹  y(xP2−P)=1  ⟹  y=1P(xP−1).xyP^2 - yP = 1 \implies y(xP^2 - P) = 1 \implies y = \frac{1}{P(xP-1)}.

Recall v=xyv = xy, u=yu = y, so x=v/ux = v/u. Rewrite in (u,v)(u,v): noting u=yu = y, v=xyv = xy: u=vP−1P.u = vP - \frac{1}{P}. This is Clairaut form with f(P)=−1/Pf(P) = -1/P.

Step 3 — General solution.

Set P=cP = c: y=cxy−1c  ⟹  c2xy−cy−1=0.y = cxy - \frac{1}{c} \implies \boxed{c^2xy - cy - 1 = 0.}

Step 4 — Singular solution.

Differentiate u=vP−1/Pu = vP - 1/P with respect to vv; branch dP/dv≠0dP/dv \ne 0 gives: 0=v+1P2  ⟹  v=−1P2.0 = v + \frac{1}{P^2} \implies v = -\frac{1}{P^2}. Also u=vP−1/P=−1/P−1/P=−2/Pu = vP - 1/P = -1/P - 1/P = -2/P, so P=−2/uP = -2/u. Substitute into v=−1/P2v = -1/P^2: v=−u24  ⟹  xy=−y24  ⟹  y2+4xy=0  ⟹  y(y+4x)=0.v = -\frac{u^2}{4} \implies xy = -\frac{y^2}{4} \implies y^2 + 4xy = 0 \implies y(y+4x)=0. Discarding y=0y=0 (trivial), the singular solution is y+4x=0\boxed{y + 4x = 0}.

Verification: On y=−4xy = -4x: p=−4p = -4. Substitute into the original: x2(16)+(−4x)(2x+(−4x))(−4)+(−4x)2=16x2+(−4x)(−2x)(−4)+16x2=16x2−32x2+16x2=0x^2(16) + (-4x)(2x + (-4x))(-4) + (-4x)^2 = 16x^2 + (-4x)(-2x)(-4) + 16x^2 = 16x^2 - 32x^2 + 16x^2 = 0. ✓\checkmark


Common Traps

Marks-Aware Writing

For a 10-mark question: Show the substitution and chain-rule conversion explicitly (2 marks), display the Clairaut form with ff identified (2 marks), state the general solution (2 marks), show the differentiation x+f′(p)=0x + f'(p) = 0 and eliminate pp (3 marks), box the singular solution (1 mark). Do not skip the “convert back to x,yx, y” step — it is a marking point.

For a 15-mark question: Everything above, plus a brief verification that the singular solution satisfies the original ODE (swap pp back in; 2–3 marks) and a one-sentence geometric interpretation (“the family of lines is tangent to the curve…”; 1–2 marks). Write the final answers in boxes.

For the 22-mark question (2019): The examiner expects (a) singular solution via discriminant, (b) full Lagrange derivation with the dX/dPdX/dP ODE written out, (c) complete primitive in final (x,y)(x, y) form, (d) geometric interpretation linking circles to their tangent-line envelope. Allocate roughly 5 + 10 + 5 + 2 marks. Show all algebra steps — no “it can be shown” shortcuts.

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