Q.If f(x)=∣tan2x∣, then find the value of f′(x) at x=3π.
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🔒 Start your 14-day free trial to unlock the full solution →Part (a)Concept understanding — Differentiability of Absolute Value
Differentiability of the Absolute Value Function
Start with something familiar: the absolute value of x, written ∣x∣, is its distance from zero on the number line. So ∣3∣=3, ∣−5∣=5, and ∣0∣=0. Graphically, it looks like a V-shape — two straight lines meeting at the origin.
Differentiability is about whether a function has a well-defined slope (derivative) at a point. For smooth curves like x2 or sinx, the slope exists everywhere. But the absolute value function has a sharp corner at x=0 — and that corner is the whole story.
Intuition: Why the corner matters
Walk along y=∣x∣ from left to right. Approaching x=0 from the left, the slope is −1 (the line goes downward). Leaving x=0 to the right, the slope is suddenly +1 (the line goes upward). At x=0, there's no single slope — it changes abruptly. That's why ∣x∣ is not differentiable at x=0. Everywhere else — for x<0 and x>0 — the graph is a straight line with constant slope, so ∣x∣ is differentiable at every point except x=0.
A function must be continuous to be differentiable, but continuity alone isn't enough. The absolute value function is continuous at x=0 (no break), yet fails to be differentiable there because of the sharp corner.
The precise statement
Let f(x)=∣x∣. Then:
- For x>0: f(x)=x, so f′(x)=1.
- For x<0: f(x)=−x, so f′(x)=−1.
- At x=0: the derivative does not exist, because the left-hand and right-hand derivatives are different numbers.
f′(0)=limh→0h∣0+h∣−∣0∣=limh→0h∣h∣
This limit does not exist because:
- From the right (h→0+): h∣h∣=hh=1
- From the left (h→0−): h∣h∣=h−h=−1
Since the two one-sided limits differ, the two-sided limit does not exist.
A common mistake is to think that because ∣x∣ is continuous at x=0, it must be differentiable there. Continuity is necessary for differentiability, but not sufficient. The absolute value function is the classic counterexample.
The bigger picture …
Part (b)Concept understanding — Chain Rule
The Chain Rule: Why It Makes Sense
Imagine you're assembling a toy. First you put part A into part B, then you put that combined piece into part C. The final toy's position depends on how you moved A, which then affected B, which then affected C. That's exactly what the chain rule captures — how a change in the first variable ripples through a sequence of functions to affect the final output.
Let's make this concrete. Suppose you have a function f that depends on g, and g itself depends on x:
y=f(g(x))
You want to know: if x changes by a tiny amount, how much does y change? The answer isn't just f′(g(x)) — because g(x) itself changes when x changes. You have to multiply the two rates:
- How fast does g change with respect to x? That's g′(x).
- How fast does f change with respect to its input g? That's f′(g(x)).
The total effect is the product:
dxdy=f′(g(x))⋅g′(x)
In Leibniz notation, this looks even more natural: dxdy=dudy⋅dxdu, where u=g(x). The du's "cancel" like fractions — though this is just a helpful memory aid, not a rigorous proof.
The Precise Statement
Chain Rule (single variable): If g is differentiable at x and f is differentiable at g(x), then the composite function h(x)=f(g(x)) is differentiable at x, and
h′(x)=f′(g(x))⋅g′(x)
That's it. One multiplication. But the power is enormous — it lets you differentiate almost any nested function.
A Simple Example
Differentiate h(x)=sin(3x2).
Here f(u)=sinu and g(x)=3x2. Then:
- f′(u)=cosu, so f′(g(x))=cos(3x2)
- g′(x)=6x
Multiply: h′(x)=cos(3x2)⋅6x=6xcos(3x2)
The most common mistake is forgetting to multiply by the inner derivative. Students often write dxdsin(3x2)=cos(3x2) and stop — that's wrong. The chain rule demands you also multiply by 6x.
Why It's Called a "Chain"
Think of a chain of links: x→g→f. Each link has its own rate of change. To find the total rate from x to f, you multiply the rates of each link. If you had three functions — say h(x)=f(g(k(x))) — you'd multiply three derivatives: …
Part (a)
f(x)=∣tan2x∣. At x=3π, tan32π=−3<0, and tan2x<0 on both sides, so locally f(x)=−tan2x.
f′(x)=−2sec22x,sec232π=(−2)2=4, …
Part (a): near x=3π, tan2x<0 so f=−tan2x and f′(3π)=−8. Part (b): y=cosec(cot−1x) simplifies to 1+x2, from which 1+x2dxdy−x=0.
Part (a)
Concept
∣u∣ has a corner only where u=0. Since tan2x=0 at x=3π, f is differentiable there, and the local sign of tan2x fixes the sign of the derivative.
Steps
- Value: 2x=32π, tan32π=−tan3π=−3 (=0).
- Sign nearby: for x just below and above 3π, 2x stays in the second quadrant where tan<0. So ∣tan2x∣=−tan2x locally.
- Differentiate: f′(x)=−2sec22x. …
Showing the 12 most recent of 124 on this concept.
- CBSE 2026Set V11 markQ.Choose from [0,3,−1,2,−2,1]. The left hand derivative of ∣x∣ with respect to x at x=0 is ____.
›Reveal solutionSolution
Just left of 0, ∣x∣=−x has slope −1, so the left-hand derivative is −1.
The left-hand derivative at x=0 is
limh→0−h∣0+h∣−∣0∣=limh→0−h−h=−1, …
- CBSE 2026Set A1 markMCQQ.dxdx2+ax+1=(a) 2x2+ax+1x+a(b) 2x2+ax+12x+a(c) x2+ax+12x+a(d) 2x2+ax+11
›Reveal solutionSolution
dxdx2+ax+1=2x2+ax+12x+a.
Let u=x2+ax+1, so dxdu=2x+a.
Using dxdu=2u1⋅dxdu: …
- CBSE 2026Set A1 markMCQQ.dxd(sinx2)=(a) 2xcosx2(b) cosx2(c) x2cosx2(d) xcosx2
›Reveal solutionSolution
dxdsin(x2)=2xcos(x2).
Let u=x2, so dxdu=2x.
By the chain rule, …
- CBSE 2026Set A1 markMCQQ.dxdcotx=(a) 2cotx1(b) csc2x(c) 2cotx−csc2x(d) 2cotxcsc2x
›Reveal solutionSolution
dxdcotx=2cotx−csc2x.
Let u=cotx, so dxdu=−csc2x.
Using dxdu=2u1⋅dxdu: …
- CBSE 2026Set A1 markMCQQ.dxd(cosx)=(a) sinx(b) 2x−sinx(c) 2xsinx(d) 2x1
›Reveal solutionSolution
dxdcosx=2x−sinx.
Let u=x, so dxdu=2x1.
By the chain rule, …
- CBSE 2026Set A1 markMCQQ.dxd(cosx3)=(a) −3x2sinx3(b) sinx3(c) 3x2sinx3(d) 3x2
›Reveal solutionSolution
Chain rule on cos(x3) gives −3x2sinx3.
Let the inner function be u=x3, so y=cosu.
…
- CBSE 2026Set ANNUAL1 markMCQQ.Write the derivative of log(cosex).(a) −tanex(b) extanex(c) −extanex(d) tanex
›Reveal solutionSolution
Using the chain rule twice, dxdlog(cosex)=−extanex.
Let y=log(cosex). We differentiate using the chain rule, working from the outside in.
Step 1: Differentiate log(u) where u=cosex:
dxdy=cosex1⋅dxd(cosex)
Step 2: Differentiate cos(v) where v=ex: …
- CBSE 2026Set ANNUAL1 markMCQQ.If y=cos−1(1+x21−x2), 0<x<1, then dxdy is equal to(a) 1+x21(b) 4+x2(c) 1+x22(d) x+x22
›Reveal solutionSolution
Put x=tanϕ so the expression simplifies to cos−1(cos2ϕ)=2ϕ=2tan−1x, whose derivative is standard.
Let x=tanϕ. Then 1+x21−x2=1+tan2ϕ1−tan2ϕ=cos2ϕ.
…
- CBSE 2026Set ANNUAL1 markQ.If y=ex+ex2+…+ex5, then find dxdy.
›Reveal solutionSolution
Differentiate each term exn using the chain rule: dxdexn=nxn−1exn.
y=ex+ex2+ex3+ex4+ex5
…
- CBSE 2026Set ANNUAL1 markMCQQ.dxd(cos3x)=(a) sin3x(b) −3sin3x(c) cos3x(d) −3cos3x
›Reveal solutionSolution
Differentiate cos(3x) using the chain rule: derivative of cosu is −sinu, times dxdu.
…
- CBSE 2026Set ANNUAL1 markMCQQ.dxdtan−1(x2)=(a) 1+x42x(b) 1+x2x(c) 1+x2x3(d) None of these
›Reveal solutionSolution
Use dxdtan−1u=1+u21⋅dxdu with u=x2.
…
- CBSE 2026Set ANNUAL1 markMCQQ.dxdesinx=(a) esinx⋅cosx(b) esinx(c) cosx(d) None of these
›Reveal solutionSolution
Differentiate eu with u=sinx: derivative is eu⋅dxdu.
…
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