Frequency: 8 sub-parts across 8 of 13 years (2013, 2014, 2015, 2016, 2018, 2020, 2022, 2025)
Priority tier: T1
Marks (count): 10 (3), 13 (2), 15 (2), 20 (1)
Average solve time: ~16 min
Difficulty mix: medium 5, hard 3
Section: B | Dominant type: computation
Why This Chapter Matters
The Cauchy-Euler (equidimensional) equation appears in 8 of the last 13 years — no year with a known UPSC result is missing it entirely. The method is a single substitution (x=et) that converts a variable-coefficient ODE into a constant-coefficient one, then the full machinery of operator methods applies. Three variants appear: standard xn, shifted (a+bx)n, and order-reduction when the y term is absent. Mastering one set of operator identities covers all of them.
Minimum Theory
Cauchy-Euler operator identities. Under x=et, t=lnx, D=d/dt:
xdxdy=Dy,x2dx2d2y=D(D−1)y,x3dx3d3y=D(D−1)(D−2)y.
In general: xny(n)=D(D−1)⋯(D−n+1)y. After substitution, the ODE has constant coefficients in t.
Generalised Cauchy-Euler. If the equation has (ax+b) instead of x: substitute ax+b=et (equivalently, t=ln(ax+b)). The operators become (ax+b)y′=aDy and (ax+b)2y′′=a2D(D−1)y — note the factors of a.
Order reduction. If the y term (zero-th order) is absent and the lowest term is xy′, substitute p=y′ to convert to a second-order Cauchy-Euler in p, then integrate once.
Resonance in the PI. After the x=et substitution, if the RHS is emt and m is a root of the auxiliary equation: multiply the trial PI by t. If m is a double root: multiply by t2. This is the standard resonance rule.
Operator formula for PI. For yp=f(D)1eat: if f(a)=0, then yp=eat/f(a). For cosbt or sinbt: replace D2→−b2 (if no cancellation). For resonance: yp=t⋅eat/f′(a).
Operator expansion. For x3y′′′: D(D−1)(D−2)=D3−3D2+2D — three terms, not just D3. Missing the lower-order terms changes the auxiliary equation.
Resonance check. After writing the constant-coefficient ODE, compare each RHS term to the CF modes. cost resonates with D2+1=0; e2t resonates with D=2. In each case, multiply the trial PI by t (or use yp=teat/f′(a)).
Shifted variables. For (ax+b)ky(k): factors of a accumulate in the derivative conversion. (3x+2)y′=3Dy but (3x+2)2y′′=9D(D−1)y. Factor of 9, not 1.
Order reduction. If there is no y term in the ODE, do NOT try to write the Cauchy-Euler operators directly on y for a cubic. Substitute p=y′ first; the resulting equation is second-order.
The third arbitrary constant in the 2016 problem enters via the final integration (not from the auxiliary equation) — easy to forget.
Back-substitution.e2t=x2, te2t=x2lnx, tcost=lnxcos(lnx). Write every term in terms of lnx and powers of x (or ax+b).
Marks-Aware Writing
10-mark questions (2020, 2022, 2025): State the substitution; write the constant-coefficient ODE; state roots; write CF; compute PI (show the operator calculation); state general solution with back-substitution. Four to five steps; don’t expand operator products in full — just state the result.
13-mark questions (2015-Q8d, 2018): Full operator expansion showing how the coefficients combine; roots; CF; PI with resonance handling shown (state f(m)=0 and use f′ formula); general solution in x.
15-mark questions (2013, 2014, 2016, 2025): Same as 13-mark plus one of: complex-method PI (2013), third-order CF with cube roots (2014), order-reduction via p=y′ (2016), shift operator for PI (2025).
20-mark questions (2014): Full operator expansion for a third-order equation, all three cube roots computed, two-step PI (operator method including the i computation), full back-substitution.
Practice Set
Year
Paper/Q
Marks
Sub-type
One-line hint
2025
P1-Q7c-ii
10
3rd order
Operator D3+1=(D+1)(D2−D+1); roots −1,21±i23; shift PI for tet
2022
P1-Q8a-ii
10
shifted (3x+2)
u=3x+2; multiply dy/dx by 3 and d2y/dx2 by 9; operator 3D2+2D−1
2020
P1-Q8a-i
10
shifted (x+1)
t=ln(x+1); D2−5D+6=(D−2)(D−3); e2t resonates; PI =−6te2t
2018
P1-Q7a
13
shifted (1+x)
t=ln(1+x); D2+1; 4cost resonates; PI =2tsint
2016
P1-Q6c
15
order reduction
No y term; p=y′; 2nd-order CE; roots 2,3; integrate to get x3,x4; c1 from integration
2015
P1-Q8d
13
4th order, double resonance
Factor D4−3D2−4=(D2−4)(D2+1); both e2t and cost resonate
2014
P1-Q6b
20
3rd order
D3+8=0: roots −2,1±i3; operator on cost: D3→−D; PI =8cost−sint
2013
P1-Q6c
15
resonant tsint
D2+1=0; tsint: complex method y=eitu; u′′+2iu′=t; PI =(tsint−t2cost)/4
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