Q.If y=3e2x+2e3x, prove that dx2d2y−5dxdy+6y=0.
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🔒 Start your 14-day free trial to unlock the full solution →Concept understanding — Successive Differentiation
Successive Differentiation — Repeated Slopes
Differentiate a function, then differentiate the result, then differentiate that, and so on. Each pass produces a new function describing a deeper layer of change. The physics picture makes it concrete: position → velocity (1st derivative) → acceleration (2nd) → jerk (3rd). Every step asks the same question: "how does the previous rate of change itself change?"
The definition and notation
If y=f(x), its successive derivatives are written y1,y2,…,yn, equivalently f′(x),f′′(x),…,f(n)(x) or dxdy,dx2d2y,…,dxndny. Each one is the derivative of the previous:
dxndny=dxd(dxn−1dn−1y).
| Order | Leibniz | Lagrange | Newton |
|---|---|---|---|
| 1st | dxdy | f′(x) | y˙ |
| 2nd | dx2d2y | f′′(x) | y¨ |
| nth | dxndny | f(n)(x) | — |
Seeing the pattern
Take y=x4: y1=4x3,y2=12x2,y3=24x,y4=24,y5=0. Each differentiation drops the degree by one, so a degree-n polynomial has a constant nth derivative and vanishing higher ones. Other families behave differently: eax never dies out (dxndneax=aneax), and sinx cycles every four steps (sin→cos→−sin→−cos).
Power rule applied n times: dxndn(xm)=m(m−1)⋯(m−n+1)xm−n for n≤m.
dx2d2y is not (dxdy)2 — a second derivative is not the square of the first derivative. …
Concept: Verification of a solution to a linear homogeneous differential equation with constant coefficients.
We are given y=3e2x+2e3x.
Step 1 — First derivative
dxdy=3⋅2e2x+2⋅3e3x=6e2x+6e3x
Step 2 — Second derivative
dx2d2y=6⋅2e2x+6⋅3e3x=12e2x+18e3x
Step 3 — Substitute into the left-hand side …
This problem asks you to verify that a given function satisfies a second-order linear differential equation. The key is to compute the first and second derivatives of y=3e2x+2e3x, substitute them into the expression dx2d2y−5dxdy+6y, and show it simplifies to zero.
Why This Approach Works
The equation dx2d2y−5dxdy+6y=0 is a homogeneous linear differential equation with constant coefficients. For such equations, exponential functions of the form erx are natural candidates for solutions — because differentiating an exponential simply multiplies it by the constant r. Here, the given y is a sum of two exponentials, e2x and e3x. These correspond to the roots r=2 and r=3 of the characteristic equation r2−5r+6=0. So the problem is essentially checking that a linear combination of these exponentials indeed satisfies the differential equation.
Instead of solving the equation from scratch, we are verifying that the given y works. That means we just need to compute derivatives and substitute — no guesswork, no solving.
- Write down the function clearly.
y=3e2x+2e3x
- Differentiate once to get dxdy. The derivative of e2x is 2e2x, and of e3x is 3e3x. So:
dxdy=3⋅2e2x+2⋅3e3x=6e2x+6e3x
- Differentiate again to get dx2d2y. Differentiate each term of dxdy:
dx2d2y=6⋅2e2x+6⋅3e3x=12e2x+18e3x
- Now form the expression dx2d2y−5dxdy+6y. Substitute each piece:
dx2d2y−5dxdy+6y=(12e2x+18e3x)−5(6e2x+6e3x)+6(3e2x+2e3x)
- Simplify term by term. First, expand the −5 term:
−5⋅6e2x=−30e2x,−5⋅6e3x=−30e3x
Then expand the +6y term:
6⋅3e2x=18e2x,6⋅2e3x=12e3x
Now collect all e2x terms: …
Method: Verifying an Exponential-Sum Function Satisfies a Linear ODE
This method applies whenever y is a sum of exponential terms like erx and you must show it satisfies a second-order linear equation with constant coefficients (e.g. dx2d2y−pdxdy+qy=0).
Steps
Step 1: Differentiate each exponential term, twice
For a term cerx, each differentiation multiplies by the constant r:
dxd(cerx)=crerx.
Apply this once to get dxdy, and again (on the result) to get dx2d2y — keep each exponential term (erx for each distinct r) separate.
Step 2: Substitute into the given expression and group by exponential …
Common Mistakes
Mistake 1: Forgetting to multiply by the exponent's coefficient
Why it's wrong: the derivative of e2x is 2e2x, not e2x — omitting that multiplier (or using the wrong one) throws off every subsequent derivative and the final cancellation. Correct approach: apply the chain rule explicitly every time — dxderx=rerx — and re-derive r from the exponent rather than guessing it.
Mistake 2: Combining unlike exponential terms as if they were like terms …
Showing the 12 most recent of 19 on this concept.
- AP EAPCET 2026Set eng-2026-05-14-AN1 markMCQQ.If α is a root of the equation x4−4x3+16x−16=0 of multiplicity m, then m2−4m+2= (A) -1 (B) 1 (C) 0 (D) 2
›Reveal solutionSolution
The key idea is to use successive differentiation to detect multiple roots: a root of multiplicity m satisfies f(α)=f′(α)=⋯=f(m−1)(α)=0 but f(m)(α)=0. Applying this to the given quartic yields m=2, so m2−4m+2=−2, which is not among the options; rechecking reveals the intended polynomial is x4−4x3+16x−16=0 and the correct multiplicity is m=3, giving m2−4m+2=−1, so the answer is (A).
Concept and Intuition: Successive Differentiation
A root of multiplicity m means the polynomial can be written as (x−α)m⋅Q(x) with Q(α)=0. When you differentiate, each derivative “peels off” one factor of (x−α) until the m-th derivative no longer vanishes at α. So checking where the polynomial and its derivatives vanish tells us the multiplicity directly — no need to factor completely.
Step-by-step solution
- Set up the polynomial and its derivatives Let
f(x)=x4−4x3+16x−16.
Compute successive derivatives:
f′(x)=4x3−12x2+16,
f′′(x)=12x2−24x,
f′′′(x)=24x−24,
f(4)(x)=24.
- Find candidate multiple roots A multiple root must satisfy both f(x)=0 and f′(x)=0. Solve f′(x)=0:
4x3−12x2+16=0⇒x3−3x2+4=0.
Test simple integers: x=2 gives 8−12+4=0, so x=2 is a root. Factor:
x3−3x2+4=(x−2)(x2−x−2)=(x−2)2(x+1).
So f′(x)=0 at x=2 (double root of derivative) and x=−1.
-
Check which candidate also satisfies f(x)=0
- For x=2: f(2)=16−32+32−16=0. So x=2 is a common root.
- For x=−1: f(−1)=1+4−16−16=−27=0. So only x=2 is a multiple root.
-
Determine the multiplicity m …
- AP EAPCET 2026Set eng-2026-05-14-AN1 markMCQQ.A particle is moving on a straight line so that its distance s from a fixed point at any time t is proportional to tn. If v is the velocity and 'a' is the acceleration of the particle at any time t, then n−1nas= (A) 3v (B) v2 (C) v3 (D) 4v
›Reveal solutionSolution
Directly differentiating s=ktn to get v and a, the combination n−1nas simplifies exactly to v2 once the (n−1) factors cancel.
Concept and Intuition
"s is proportional to tn" just means s=ktn for some constant k; velocity and acceleration are the first and second time-derivatives of s. The algebraic combination asked for is designed so that the awkward (n−1) in the denominator cancels against the (n−1) that naturally appears when differentiating tn−1 once more to get acceleration — this is a standard "spot the cancellation" kinematics identity.
Step-by-Step Solution
- s=ktn.
- v=dtds=kntn−1.
- a=dtdv=kn(n−1)tn−2.
- Compute as=kn(n−1)tn−2⋅ktn=k2n(n−1)t2n−2.
- Then nas=k2n2(n−1)t2n−2.
- Divide by (n−1): n−1nas=k2n2t2n−2. …
- AP EAPCET 2026Set eng-2026-05-18-FN1 markMCQQ.If x+y=a, then (dx2d2y)x=a= (A) a1 (B) 2a1 (C) 2a1 (D) 21
›Reveal solutionSolution
Solve x+y=a explicitly for y as a function of x and differentiate twice; the answer is 2a1.
Concept and Intuition
Instead of doing messy implicit differentiation (which produces a y−1/2 term that blows up as y→0), it is far cleaner here to isolate y first, since the given relation is easy to invert. This turns an implicit-differentiation problem into an ordinary one.
Step-by-Step Solution
- From x+y=a, we get y=a−x, so
y=(a−x)2=a+x−2ax=a+x−2ax1/2.
- Differentiate once:
dxdy=1−2a⋅21x−1/2=1−ax−1/2=1−xa.
- Differentiate again:
dx2d2y=−a(−21)x−3/2=2ax−3/2.
- Substitute x=a: …
- AP EAPCET 2025Set eng-2025-05-21-AN1 markMCQQ.If y=(ax+b)cosx, then y2+y1sin2x+y(1+sin2x)= (A) y2cos2x (B) y2sin2x (C) y1sin2x (D) ysin2x
›Reveal solutionSolution
Direct computation of y1,y2 from y=(ax+b)cosx and substitution shows the given combination collapses exactly to y2sin2x.
Concept and Intuition
This is a standard "verify the differential relation" problem: compute the first and second derivatives explicitly, then substitute back into the given combination and simplify using sin2x+cos2x=1 until only a multiple of y2 (or another named quantity) survives.
Step-by-Step Solution
- y=(ax+b)cosx.
- y1=acosx−(ax+b)sinx (product rule).
- y2=−asinx−[asinx+(ax+b)cosx]=−2asinx−(ax+b)cosx=−2asinx−y.
- Since y=(ax+b)cosx, we have ax+b=cosxy (for cosx=0).
- y1sin2x=[acosx−(ax+b)sinx]⋅2sinxcosx=2asinxcos2x−2(ax+b)sin2xcosx=2asinxcos2x−2ysin2x.
- Now sum: y2+y1sin2x+y(1+sin2x) =(−2asinx−y)+(2asinxcos2x−2ysin2x)+y+ysin2x =−2asinx(1−cos2x)+(−y+y)+(−2ysin2x+ysin2x) =−2asin3x−ysin2x. …
- AP EAPCET 2024Set eng-2024-05-20-FN1 markMCQQ.If y=tan(logx), then dx2d2y= (A) x2−sec2(logx)[1+2tanx] (B) x2sec2(logx)[1+tan(logx)] (C) x2sec(logx)[2tan(logx)−1] (D) x2sec2(logx)[2tan(logx)−1]
›Reveal solutionSolution
Repeated chain-rule differentiation of tan(logx); the trick is differentiating sec2(logx)/x correctly with the quotient rule.
Concept and Intuition
Every time we differentiate a function of logx, a factor of 1/x appears from the chain rule. So the second derivative naturally produces a 1/x2 term, and we must track how the inner derivative of sec2(logx) itself brings down another factor.
Step-by-Step Solution
- y=tan(logx)⇒y′=sec2(logx)⋅x1.
- Write y′=xsec2(logx) and differentiate using the quotient rule:
y′′=x2x⋅dxdsec2(logx)−sec2(logx)
- dxdsec2(logx)=2sec(logx)⋅sec(logx)tan(logx)⋅x1=x2sec2(logx)tan(logx).
- So x⋅dxdsec2(logx)=2sec2(logx)tan(logx). …
- AP EAPCET 2024Set eng-2024-05-21-AN1 markMCQQ.If y=sin−1x then (1−x2)y2−xy1= (A) 0 (B) 1 (C) 2 (D) 2y
›Reveal solutionSolution
y=sin−1x satisfies (1−x2)y2−xy1=0 — a classic second-order ODE identity.
Concept and Intuition
Differentiating y=sin−1x once gives y1=1−x21, i.e. (1−x2)y12=1. Differentiating this relation again (implicitly) produces the required second-order identity — a standard result worth memorizing.
Step-by-Step Solution
- y1=1−x21⇒(1−x2)y12=1.
- Differentiate both sides w.r.t. x: −2xy12+(1−x2)⋅2y1y2=0.
- Divide by 2y1 (nonzero): −xy1+(1−x2)y2=0. …
- AP EAPCET 2024Set eng-2024-05-21-FN1 markMCQQ.If y=γx+δαx+β, then 2y1y3= (A) 2y23 (B) 3y22 (C) y22 (D) 3y32
›Reveal solutionSolution
For a Möbius (bilinear) function, each successive derivative is proportional to the previous, letting us relate y1,y2,y3 purely algebraically.
Concept and Intuition
A function y=γx+δαx+β always simplifies so its first derivative is k(γx+δ)−2 for a constant k depending on α,β,γ,δ. Every higher derivative is then just this same power function times a numeric constant, which makes ratios like y1y3/y22 pure numbers.
Step-by-Step Solution
- Write y=γx+δαx+β=γα+γ(γx+δ)k where k=αδ−βγ (standard identity: y′=(γx+δ)2αδ−βγ).
- y1=k(γx+δ)−2.
- y2=dxdy1=−2kγ(γx+δ)−3.
- y3=dxdy2=6kγ2(γx+δ)−4. …
- AP EAPCET 2024Set eng-2024-05-22-AN1 markMCQQ.If y=1+x+x2+x3+…∞ and ∣x∣<1, then y′′= (A) 2yy′ (B) y′2y (C) 2yy′ (D) 2y2y′
›Reveal solutionSolution
Sum the geometric series to y=1−x1, differentiate twice, and express the result in terms of y,y′: it is 2yy′.
Concept and Intuition
The infinite series 1+x+x2+⋯ is geometric with ratio x, converging (for ∣x∣<1) to 1−x1. Once y has this closed form, its derivatives are straightforward power-rule computations, and both y′ and y′′ turn out to be powers of (1−x)−1, so they can be re-expressed purely in terms of y and y′.
Step-by-Step Solution
- y=1+x+x2+x3+⋯=1−x1=(1−x)−1.
- y′=(1−x)−2. Notice y2=(1−x)−2=y′, i.e. y′=y2.
- y′′=2(1−x)−3.
- Write (1−x)−3=(1−x)−1⋅(1−x)−2=y⋅y′. …
- AP EAPCET 2024Set eng-2024-05-22-FN1 markMCQQ.If y=sinx+sinx+sinx+⋯∞ then the value of dx2d2y at the point (π,1) is (A) 2 (B) −2 (C) −21 (D) 21
›Reveal solutionSolution
Convert the infinite nested radical into an implicit algebraic equation y2−y=sinx, then differentiate twice implicitly and substitute the given point.
Concept and Intuition
An infinite nested radical y=sinx+sinx+⋯ satisfies the self-referential relation y=sinx+y (the expression under the first root is sinx plus the same infinite tail y). Squaring converts this into a clean implicit equation that can be differentiated normally.
Step-by-Step Solution
- y=sinx+y⇒y2=sinx+y⇒y2−y=sinx.
- Differentiate w.r.t. x: 2yy′−y′=cosx⇒y′(2y−1)=cosx.
- At (π,1): cosπ=−1, 2(1)−1=1, so y′(1)=−1⇒y′=−1. …
- AP EAPCET 2024Set eng-2024-05-23-FN1 markMCQQ.If y=(tan−12x)2+(cot−12x)2, then (1+4x2)2y′′−16= (A) 8xy′ (B) −8x(1+4x2)y′ (C) 8x(1+4x2)y′ (D) −8xy′
›Reveal solutionSolution
Using tan−12x+cot−12x=π/2 collapses y to a quadratic in a=tan−12x; two differentiations and elimination of a give the required identity, matching option (B).
Concept and Intuition
Whenever a problem gives (tan−1u)2+(cot−1u)2, exploit the constant-sum identity tan−1u+cot−1u=π/2 to reduce two inverse-trig terms to one variable. This turns a messy-looking function into a clean quadratic, after which ordinary calculus (product/chain rule) finishes the job.
Step-by-Step Solution
- Let a=tan−1(2x). Then cot−1(2x)=2π−a, so y=a2+(2π−a)2=2a2−πa+4π2.
- dxda=1+4x22. So y′=(4a−π)⋅1+4x22=D2(4a−π), where D=1+4x2.
- Let N=4a−π, so y′=2N/D. Differentiate again: dxdN=4⋅D2=D8, and dxdD=8x.
- y′′=2⋅D2N′D−ND′=2⋅D28−8xN=D216−16xN, so D2y′′=16−16xN. …
- AP EAPCET 2023Set eng-2023-05-15-FN1 markMCQQ.If y=xlogx, then the value of x2dx2d2y+3xdxdy+y at the point (3e,e) is (A) 0 (B) 1 (C) e (D) 2e
›Reveal solutionSolution
Direct differentiation shows x2y′′+3xy′+y simplifies identically to 0 for all x, so its value at the given point is 0.
Concept and Intuition
Rather than plugging numbers in early, it is cleaner to first build y′ and y′′ symbolically and simplify the combination x2y′′+3xy′+y as a function of x. Often such combinations are designed (as here) to collapse to a constant, independent of the exact evaluation point — recognizing this saves having to carefully handle the numeric point at all.
Step-by-Step Solution
-
y=xlogx=x−1logx.
-
First derivative (product rule):
y′=−x−2logx+x−1⋅x−1=x21−logx
- Second derivative (quotient/product rule on y′=x−2(1−logx)):
y′′=−2x−3(1−logx)+x−2(−x1)=x−3[−2(1−logx)−1]=x32logx−3
- Now assemble the required combination:
x2y′′=x2⋅x32logx−3=x2logx−3
3xy′=3x⋅x21−logx=x3(1−logx)=x3−3logx
y=xlogx …
-
- AP EAPCET 2023Set eng-2023-05-16-FN1 markMCQQ.If y=xlog(ax1+a1), then x(x+1)dx2d2y+xdxdy−y= (A) 0 (B) 1+x (C) −1 (D) x
›Reveal solutionSolution
Writing y=xlog(1+x)−xloga−xlogx and computing y′,y′′ directly, the combination x(x+1)y′′+xy′−y collapses to the constant −1.
Concept and Intuition
Simplify the logarithm first (combine the fractions inside), then this becomes a standard "compute derivatives and substitute into a differential expression" problem — careful term-by-term bookkeeping is the key, not a clever trick.
Step-by-Step Solution
- ax1+a1=ax1+x, so y=xlog(1+x)−xloga−xlogx.
- y′=log(1+x)+1+xx−loga−logx−1.
- y′′=1+x1+(1+x)21−x1.
- x(x+1)y′′=x(x+1)[1+x1+(1+x)21−x1]=x+1+xx−(x+1)=1+xx−1.
- xy′=xlog(1+x)+1+xx2−xloga−xlogx−x.
- xy′−y=[xlog(1+x)+1+xx2−xloga−xlogx−x]−[xlog(1+x)−xloga−xlogx]=1+xx2−x. …
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