Q.Find the second order derivative of the function: x20
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.
Why it matters
Higher derivatives power the second-derivative test for maxima and minima, Taylor and Maclaurin expansions, Leibniz's theorem for the nth derivative of a product, and differential equations such as F=ma (a second derivative of position).
Successive (higher-order) differentiation is its own named section in the NCERT Class 12 Continuity and Differentiability chapter, and finding a general nth-derivative pattern for polynomials, exponentials or sine is a recurring CBSE board and JEE Main question type. Students searching 'successive differentiation class 12 examples' or 'nth derivative formula' will recognize this repeated-differentiation notation (y₁, y₂, ..., yₙ) as the standard exam convention.
Differentiate x20 twice using the power rule dxdxn=nxn−1 — this is successive (repeated) differentiation.
First derivative:
dxdy=20x19
Second derivative — differentiate the result again:
dx2d2y=20⋅19x18=380x18
dx2d2y=380x18
Applying the power rule twice to x20 gives dx2d2y=380x18.
A second-order derivative just means we differentiate, then differentiate the result again. For a pure power of x the only tool we need is the power rule, dxdxn=nxn−1 — no chain rule, no product rule.
Step 1 — First derivative
For y=x20,
dxdy=20x20−1=20x19.
Step 2 — Second derivative
Now differentiate 20x19. The constant 20 stays put; apply the power rule to x19:
dx2d2y=20⋅19x19−1=20⋅19x18.
Step 3 — Simplify
Since 20×19=380,
dx2d2y=380x18.
In one shot, dx2d2xn=n(n−1)xn−2. With n=20: 20⋅19=380 and the exponent drops to 18.
dx2d2y=380x18
Method: Successive Differentiation of a Power Function
This method finds a second (or higher) order derivative of a pure power xn by applying the power rule repeatedly, one order at a time.
Steps
Step 1: Identify the function type and the order of derivative required
Check whether the expression is a pure power of x (possibly with a constant coefficient). For a pure power, no chain rule, product rule, or quotient rule is needed — only the power rule, applied as many times as the required order.
dxd(xn)=nxn−1
Step 2: Differentiate once to get the first derivative
Apply the power rule to the original function to obtain y1=dxdy. This reduces the exponent by 1 and multiplies by the original exponent.
Step 3: Differentiate the result again for the second derivative
Treat y1 as a new function and apply the power rule to it directly — differentiate the coefficient-power expression, not the original function. This gives y2=dx2d2y.
Step 4: Simplify the constant multiplier
Multiply out any numerical coefficients that arise from repeated application (e.g., n(n−1)) and leave the answer as a single coefficient times a power of x. For higher orders, keep repeating Steps 2–3, tracking how the exponent decreases and the coefficient grows by successive multiplication.
Common Mistakes
Mistake 1: Stopping after computing only the first derivative
Why it's wrong: the question asks for the second order derivative, but 20x19 is only an intermediate step. Correct approach: always re-read what order is asked, and explicitly differentiate the first-derivative expression once more before writing the final answer.
Mistake 2: Forgetting to multiply the existing coefficient into the new one
Why it's wrong: when differentiating 20x19, both the coefficient 20 and the exponent 19 must be multiplied together (giving 380) — some students only bring down the exponent and forget to multiply it by the coefficient already present. Correct approach: apply the power rule to the whole term as 20⋅19x18, not just x18.
Mistake 3: Confusing dx2d2y with (dxdy)2
Why it's wrong: squaring the first derivative gives a completely different (and wrong) expression — the second derivative is the derivative of the derivative, not its square. Correct approach: always compute the second derivative by differentiating the first-derivative expression again, never by squaring it.
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
Since f(2)=0 and f′(2)=0, m≥2. Check f′′(2)=12(4)−24(2)=48−48=0, so m≥3.
Check f′′′(2)=24(2)−24=24=0. Hence the first non‑vanishing derivative at x=2 is the third, so multiplicity m=3.
TipA quick check: if m=3, then f(x) should have (x−2)3 as a factor. Indeed, dividing f(x) by (x−2)3=x3−6x2+12x−8 gives quotient x+2 and remainder 0, confirming f(x)=(x−2)3(x+2).
-
Compute the required expression
m2−4m+2=32−4⋅3+2=9−12+2=−1.
Watch outA common mistake is to stop after finding f′(2)=0 and assume m=2. Always check higher derivatives until you find a non‑zero one — here the second derivative also vanishes, so the multiplicity is higher.
✓Final answerThe correct option is (A).
ANSWER: A
- 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.
- Compare with v2=(kntn−1)2=k2n2t2n−2 — identical.
- So n−1nas=v2.
Common Mistakes
- Forgetting the extra factor of (n−1) that appears when differentiating v to get a (a common slip is writing a=kntn−2, dropping the (n−1) factor).
- Not recognizing that the (n−1) in the denominator is meant to cancel exactly with the one from a's formula.
✓Final answerThe correct option is (B) — v2.
ANSWER: B
- 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:
(dx2d2y)x=a=2a⋅a−3/2=2a1.
Common Mistakes
- Attempting implicit differentiation and evaluating the resulting formula at x=a,y=0 directly — this hits a 0/0-type indeterminate form because y−1/2 diverges; converting to explicit form avoids this entirely.
- Sign errors when differentiating x−1/2 twice.
✓Final answerThe correct option is (B) — 2a1.
ANSWER: B
- 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.
- From step 3, 2asinx=−(y2+y), so −2asin3x=sin2x⋅2asinx⋅(−1)⋅(−1)... more directly: −2asin3x=sin2x⋅(−2asinx)=sin2x(y2+y).
- So the total =sin2x(y2+y)−ysin2x=y2sin2x+ysin2x−ysin2x=y2sin2x.
Common Mistakes
- Sign slips in the product-rule expansion of y2 (easy to lose the −y term).
- Not substituting (ax+b)=y/cosx and instead trying to keep a,b as separate free parameters, which never lets the answer reduce to a pure y,y1,y2 expression.
✓Final answerThe correct option is (B) — y2sin2x.
ANSWER: B
- 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).
- y′′=x22sec2(logx)tan(logx)−sec2(logx)=x2sec2(logx)[2tan(logx)−1].
Common Mistakes
- Forgetting the extra 1/x that comes from differentiating sec2(logx) again (missing the chain rule the second time).
- Sign error: writing 1−2tan(logx) instead of 2tan(logx)−1.
✓Final answerThe correct option is (D) — x2sec2(logx)[2tan(logx)−1].
ANSWER: D
- 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.
- Hence (1−x2)y2−xy1=0.
Common Mistakes
- Forgetting to divide by 2y1 and leaving an extra factor of y1.
- Confusing this with the y=cos−1x version (same identity, since the sign difference cancels).
✓Final answerThe correct option is (A) — 0.
ANSWER: A
- 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.
- Compute 2y1y3=2⋅k(γx+δ)−2⋅6kγ2(γx+δ)−4=12k2γ2(γx+δ)−6.
- Compute y22=4k2γ2(γx+δ)−6.
- Therefore 2y1y3=12k2γ2(γx+δ)−6=3⋅(4k2γ2(γx+δ)−6)=3y22.
Common Mistakes
- Miscounting the power of (γx+δ) or the numeric coefficient at each differentiation step.
- Forgetting the factor of 2 on the left side when comparing to y22.
✓Final answerThe correct option is (B) — 3y22.
ANSWER: B
- 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′.
- So y′′=2yy′.
Common Mistakes
- Forgetting the series only converges (and the formula only holds) for ∣x∣<1 — irrelevant to the algebra here but worth noting.
- Arithmetic slip in matching exponents when rewriting (1−x)−3 as a product of y and y′.
✓Final answerThe correct option is (A) — 2yy′.
ANSWER: A
- 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.
- Differentiate again: dxd[y′(2y−1)]=−sinx⇒y′′(2y−1)+y′(2y′)=−sinx, i.e. y′′(2y−1)+2(y′)2=−sinx.
- At (π,1) with y′=−1: y′′(1)+2(1)=−sinπ=0⇒y′′+2=0⇒y′′=−2.
Common Mistakes
- Forgetting to apply the product rule correctly to y′(2y−1) when differentiating a second time (missing the 2(y′)2 term).
- Sign slip with sinπ=0 vs cosπ=−1.
✓Final answerThe correct option is (B) — −2.
ANSWER: B
- 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.
- Since N=2y′D, we get 16xN=8xDy′, so D2y′′=16−8xDy′.
- Therefore (1+4x2)2y′′−16=D2y′′−16=−8xDy′=−8x(1+4x2)y′.
Common Mistakes
- Trying to differentiate (tan−12x)2 and (cot−12x)2 separately without using the complementary-angle identity — it works but is far more error-prone.
- Sign slips when differentiating N=4a−π and D=1+4x2 a second time.
✓Final answerThe correct option is (B) — −8x(1+4x2)y′.
ANSWER: B
- 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
- Adding all three, the numerators combine as:
(2logx−3)+(3−3logx)+logx=(2−3+1)logx+(−3+3)=0
So
x2y′′+3xy′+y=x0=0
for every x>0 — in particular at x=3e.
Common Mistakes
- Mis-differentiating the quotient logx/x and dropping a sign, which prevents the logx terms from cancelling.
- Substituting the numeric point too early, before simplifying algebraically — this makes the cancellation much harder to spot.
✓Final answerThe correct option is (A) — 0.
ANSWER: A
-
- 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.
- Total: (1+xx−1)+(1+xx2−x)=1+xx+x2−1−x=x−1−x=−1.
Common Mistakes
- Forgetting to combine ax1+a1 into a single fraction before differentiating, making the algebra much messier.
- Sign slips when combining the xy′ and −y terms since many terms cancel and it's easy to drop one.
✓Final answerThe correct option is (C) — −1.
ANSWER: C
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