UPSC 2026 Maths Optional Paper 1 Q4b — Step-by-Step Solution
15 marks · Section A
Curve tracing (cartesian and polar) · Calculus · asked 3× in 14 yrs · Read the full method →
Question
Trace the curve y2(a+x)=x2(3a−x).
Technique
Run the standard tracing checklist on the cubic F(x,y)≡y2(a+x)−x2(3a−x)=0: symmetry, intercepts, region of existence from y2=a+xx2(3a−x)≥0, singular points (the origin is a double point — classify it by the discriminant H2−AB of the lowest-degree terms), asymptotes (coefficient of the highest power of y; then ϕ3(m) for oblique ones), and turning points from dxd(y2)=0. Each item is one bold step so every mark is separately visible to the examiner.
Solution
Throughout take a>0 (the constant is understood to be a positive length; the case a<0 is the mirror image x↦−x, and a=0 degenerates the equation to y2=−x2, i.e. the single point at the origin). Write
F(x,y)=y2(a+x)−x2(3a−x)=ay2+xy2−3ax2+x3=0.
Step 1 — Symmetry.
y occurs only through y2, so F(x,−y)=F(x,y): the curve is symmetric about the x-axis.
It is not symmetric about the y-axis (F(−x,y)=ay2−xy2−3ax2−x3=F(x,y)), nor about the origin, nor about y=x. So only the upper half need be traced; the lower half is its reflection.
Step 2 — Solve for y2 and find the region of existence.
y2=a+xx2(3a−x).(∗)
Since x2≥0, real points require a+x3a−x≥0 (or x=0).
Region
3a−x
a+x
a+xx2(3a−x)
Real y?
x<−a
+
−
−
no
x=−a
+
0
undefined
no (asymptote)
−a<x<0
+
+
+
yes
x=0
+
+
0
yes, y=0
0<x<3a
+
+
+
yes
x=3a
0
+
0
yes, y=0
x>3a
−
+
−
no
Hence the curve exists only for −a<x≤3a. It lies entirely in the vertical strip between the line x=−a (excluded) and the line x=3a (attained).
Step 3 — Intercepts.
With the x-axis: put y=0 in F=0: x2(3a−x)=0⇒x=0 (a repeated root) or x=3a. So the curve meets the x-axis at O(0,0) and at A(3a,0); the double root at x=0 already signals that the origin is a singular point.
With the y-axis: put x=0: ay2=0⇒y=0. The origin is the only intersection.
There is no other point on the axes.
Step 4 — Singular points; nature of the origin.
Fx=y2−6ax+3x2,Fy=2y(a+x).
A point is singular iff F=Fx=Fy=0.
Fy=0 gives y=0 or x=−a; but x=−a carries no point of the curve (Step 2), so y=0. Then F=0 forces x2(x−3a)=0, i.e. x=0 or x=3a.
At (3a,0): Fx=0−18a2+27a2=9a2=0, so this is an ordinary (non-singular) point.
At (0,0): Fx=0 and Fy=0, so the origin is a double point — the only singular point of the curve.
Classification. At a double point the tangents are given by the lowest-degree (here degree-two) terms of F:
ay2−3ax2=0⟹y2=3x2⟹y=±3x(two tangents at O).
Applying the standard criterion: writing the degree-two part as Ax2+2Hxy+By2 we have A=−3a, H=0, B=a, so
H2−AB=0−(−3a)(a)=3a2>0.
H2−AB>0⇒two distinct real tangents⇒ the origin is a node.
(This is consistent with Step 2: real branches of the curve exist on both sides of x=0, so the origin cannot be an isolated point; and the two tangents are distinct, so it is not a cusp.) The tangents make angles ±60∘ with the x-axis, since tan−13=60∘.
Step 5 — Tangent at A(3a,0).
At an ordinary point the tangent is Fx(x−3a)+Fy(y−0)=0. Here Fx=9a2, Fy=0, so
9a2(x−3a)=0⟹x=3a.
The tangent at A(3a,0) is vertical: the curve meets the x-axis at right angles there and turns back, which is exactly what closes the loop.
Step 6 — Asymptotes.
Parallel to the y-axis. Regard F=0 as a polynomial in y:
(a+x)y2+(x3−3ax2)=0.
Equating the coefficient of the highest power of y to zero: a+x=0, i.e.
x=−a
is a vertical asymptote. (Confirming directly from (∗): as x→−a+, the numerator →a2⋅4a=4a3>0 while a+x→0+, so y2→+∞ and y→±∞.)
Parallel to the x-axis. The coefficient of the highest power of x (namely x3) is the constant 1=0, so there is no horizontal asymptote.
Oblique. The degree-three homogeneous part of F is
F3=x3+xy2=x(x2+y2).
Put y=mx: ϕ3(m)=F3(1,m)=1+m2. Since 1+m2>0 for every real m, ϕ3 has no real root, so there is no oblique asymptote. (The factorisation x(x2+y2) shows the three asymptotic directions: the real one x=0 — which produced the vertical asymptote x=−a — and the two imaginary ones y=±ix through the circular points at infinity.)
Setting dxdy=0: x=0 or x=±3a. Of these, x=−3a<−a is outside the region of existence, and x=0 is the node (where (†) is 0/0 and Step 4 gives the two tangents instead). The genuine turning point is
Sign of (†) (monotonicity), noting (a+x)2>0 and taking the upper branch y>0:
Interval
x
3a2−x2
dy/dx
upper branch
−a<x<0
−
+
−
decreasing (falls from +∞ to 0)
0<x<3a
+
+
+
increasing (0 up to 1.180a)
3a<x<3a
+
−
−
decreasing (1.180a down to 0)
So on the upper half there is exactly one maximum, at (3a,a63−9), and by symmetry one minimum at (3a,−a63−9).
Step 8 — Table of points (take a=1; scale by a in general).
x
−0.99
−0.9
−0.5
−0.25
0
0.5
1
3≈1.732
2
2.5
2.9
3
y2
391.06
31.59
1.75
0.2708
0
0.4167
1
1.3923
1.3333
0.8929
0.2156
0
±y
19.78
5.621
1.323
0.5204
0
0.6455
1
1.1800
1.1547
0.9449
0.4644
0
(Each entry is (∗) evaluated directly; e.g. x=1: y2=21⋅2=1, and indeed y2(a+x)=1⋅2=2=x2(3a−x). ✓)
Step 9 — The traced curve.
Assembling Steps 1–8:
The curve lies wholly in the strip −a<x≤3a and is symmetric about the x-axis.
A loop in 0≤x≤3a: starting at the node O along the tangent y=3x (rising at 60∘), the upper arc climbs to the highest point (3a,a63−9)≈(1.732a,1.180a), then falls and meets the x-axis perpendicularly at A(3a,0). Its mirror image below the axis returns to O along y=−3x. The two arcs together form a closed loop of width 3a and greatest height ≈1.18a, bulging to the right of centre (its widest point is at x=3a≈1.732a=0.577×3a, i.e. right of the loop’s mid-abscissa 1.5a).
Two infinite branches in −a<x<0: from the node O, one arc leaves along y=−3x into the second quadrant, rising monotonically to +∞ as x→−a+; its mirror image leaves along y=+3x into the third quadrant, falling to −∞. Both hug the vertical asymptote x=−a, which they never meet.
The two branch-pairs cross transversally at the origin — that crossing is the node, with the loop’s tangents and the infinite branches’ tangents being the same pair of lines y=±3x.
The whole figure looks like a loop to the right of the origin with a pair of horns opening leftwards to infinity against x=−a. (This cubic is the classical trisectrix of Maclaurin.)
Figure specification (what the sketch must carry to earn the marks — these are the mathematical contents, not decoration):
Axes with O marked, and the points A(3a,0) and (−a,0) labelled on the x-axis.
The vertical asymptote x=−a drawn dashed, with both infinite branches approaching it, one to +∞ and one to −∞, and never touching it.
The two tangent lines y=±3x at the origin drawn dashed and short, labelled, so the node is unmistakable; the four arcs must visibly leave O along them at ±60∘.
The loop closed at A(3a,0) with a visibly vertical tangent there.
The turning points (3a,±a63−9) marked with a dot and labelled; the loop’s maximum height must sit at x=3a≈1.732a, which is right of the loop’s mid-abscissa 1.5a — the loop is visibly skewed towards A(3a,0), not symmetric about x=1.5a.
Nothing drawn for x<−a or x>3a — the empty regions are part of the answer.
Answer
Curve traced (a>0):y2=a+xx2(3a−x)(trisectrix of Maclaurin).Symmetric about the x-axis;exists only for −a<x≤3a.Meets the axes at O(0,0)andA(3a,0);tangent at A is x=3a(vertical).Ois a node(H2−AB=3a2>0)with tangents y=±3x.Only asymptote: x=−a(no oblique, since ϕ3(m)=1+m2 has no real root).Turning points (3a,±a63−9)≈(1.732a,±1.180a).Shape: a closed loop from O to A(3a,0),plus two branches from Orunning to ±∞against x=−a.We post more of this — worked solutions, CSAT trap breakdowns, guide chapters — a few times a week on Telegram. Free, no sign-in.Join→
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