Q.Find the second order derivative of the function: logx
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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. …
The key idea is that the second derivative of logx is found by differentiating the first derivative, using the standard derivative of the natural logarithm.
Step 1: Let y=logx (natural logarithm). The first derivative is:
dxdy=x1
Step 2: Differentiate dxdy with respect to x to get the second derivative:
dx2d2y=dxd(x1) …
The second derivative of logx is found by differentiating twice using the standard derivative of the natural logarithm. The result is −x21.
We are asked for the second order derivative of logx. In calculus, when the base of the logarithm is not specified, and the context is standard differentiation, logx almost always means the natural logarithm, lnx. This is the convention in most Indian exam syllabi (CBSE, JEE, etc.). If the base were 10, it would usually be written as log10x or explicitly stated.
The core idea is straightforward: the second derivative is simply the derivative of the first derivative. So we differentiate once, then differentiate that result.
1. First derivative of logx
The derivative of lnx with respect to x is a fundamental result:
dxd(logx)=x1
This comes from the definition of the natural logarithm as the inverse of the exponential function. If y=lnx, then ey=x, and differentiating implicitly gives eydxdy=1, so dxdy=ey1=x1.
A quick way to remember: the derivative of ln(function) is function1×derivative of function. Here the function is just x, so it's x1⋅1=x1.
2. Second derivative
Now we differentiate x1 with respect to x. It is often easier to rewrite x1 as x−1 before differentiating.
dxd(x1)=dxd(x−1)
Using the power rule dxd(xn)=nxn−1:
dxd(x−1)=(−1)x−1−1=−x−2 …
Method: Successive Differentiation of a Logarithmic Function
This method finds a higher-order derivative of a natural-logarithm expression by first reducing it to its known first-derivative form, then differentiating that result using the power rule.
Steps
Step 1: Recall the standard derivative of the logarithm
For the natural logarithm, memorise the base result:
dxd(logx)=x1,x>0
This single fact converts a logarithmic differentiation problem into an ordinary power-rule problem after the first step.
Step 2: Rewrite the first derivative as a power of x
Express x1 as x−1 so that the power rule can be applied directly for the next differentiation. …
Common Mistakes
Mistake 1: Dropping the negative sign when differentiating x1
Why it's wrong: rewriting x1 as x−1 and applying the power rule gives (−1)x−2=−x21 — the negative sign comes directly from the negative exponent and is easy to drop by accident. Correct approach: always carry the exponent's sign through explicitly, and sanity-check that 1/x has negative slope for x>0, so its derivative must be negative.
Mistake 2: Ignoring the domain restriction x>0
Why it's wrong: logx (natural log) is only defined for positive x, so both its first and second derivatives inherit that same restriction — stating the answer as valid "for all x" is technically incorrect. Correct approach: report dx2d2y=−x21 as valid for x>0 only. …
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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