Q.If y=(cosx)(cosx)(cosx)⋯∞, show that dxdy=ylogcosx−1y2tanx.
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Implicit Differentiation
When y isn't alone
You can differentiate y=x2+3x term by term because y is written explicitly in terms of x. But an equation like x2+y2=25, or x3+y3=6xy, does not give y by itself — solving for y is messy or downright impossible.
Implicit differentiation finds dxdy without isolating y: treat y as an unknown function of x, differentiate the whole equation as it stands, then solve for dxdy.
The one key move: y is really y(x)
Wherever y appears, picture y(x) hiding inside. Differentiating a y-term therefore needs the chain rule, which tacks on a factor of dxdy:
dxd(y2)=2ydxdy.
That extra dxdy on every y-term is the whole trick.
The procedure
- Differentiate both sides with respect to x, treating y as y(x).
- Each time you differentiate a y-term, multiply by dxdy (chain rule); use the product rule on mixed terms such as xy.
- Gather all dxdy terms on one side, everything else on the other.
- Factor out dxdy and divide.
Worked example
For x2+y2=25:
2x+2ydxdy=0⇒dxdy=−yx.
The answer naturally contains both x and y — that is normal here. To get the slope at a point on the curve, substitute the coordinates after differentiating; there is no need to solve for y first. …
Concept: Implicit Differentiation — the infinite tower means y=(cosx)y.
Step 1: Write the given infinite power tower as
y=(cosx)y.
Step 2: Take natural logarithms on both sides:
logy=ylog(cosx).
Step 3: Differentiate implicitly with respect to x:
y1dxdy=dxdylog(cosx)+y⋅cosx−sinx.
Step 4: Simplify using tanx=cosxsinx and collect dxdy terms:
y1dxdy−log(cosx)dxdy=−ytanx
⇒dxdy(y1−log(cosx))=−ytanx …
This is an infinite power tower of cosx, which converges for certain values. Using the property y=(cosx)y, we take logs, differentiate implicitly, and rearrange to get dxdy=ylogcosx−1y2tanx.
The key insight: when you see an infinite tower like aaa⋯, it means the exponent is the same expression all over again. So if y equals the whole tower, then y also equals (cosx)y. This self-referential equation is the heart of the solution — it lets us avoid dealing with the infinite chain directly.
Let’s walk through it.
- Set up the self-referential equation Since the tower goes on forever, the exponent of the first cosx is itself the entire tower. Therefore:
y=(cosx)y
This is valid only where the tower converges (typically for e−e≤cosx≤e1/e, but we assume the domain is such that the expression is well-defined).
- Take the natural logarithm of both sides This brings the exponent down:
logy=ylog(cosx)
Notice: log(cosx) is defined when cosx>0, which is a natural domain restriction.
- Differentiate implicitly with respect to x
Both sides are functions of x, and y is a function of x. Differentiate:
- Left side: dxdlogy=y1⋅dxdy
- Right side: use the product rule on y⋅log(cosx):
dxd[ylog(cosx)]=dxdy⋅log(cosx)+y⋅cosx1⋅(−sinx)
The derivative of $\log(\cos x)$ is $\frac{-\sin x}{\cos x} = -\tan x$.
So we have:
y1dxdy=dxdylog(cosx)−ytanx
- Collect terms with dxdy Bring the dxdylog(cosx) term to the left:
y1dxdy−dxdylog(cosx)=−ytanx
Factor out dxdy:
dxdy(y1−log(cosx))=−ytanx
- Solve for dxdy Multiply both sides by y to clear the fraction inside the bracket: …
Method: Solving Infinite Power Towers by Self-Reference
Use this method for any expression of the form y=a(x)a(x)a(x)⋯ (an infinite exponent tower). The trick is recognising that the tower, being infinite, repeats itself inside its own exponent.
Steps
Step 1: Replace the infinite tower with a self-referential equation
Since the tower never ends, the exponent on the very first factor is itself the entire tower — which is just y again:
y=a(x)y
For this problem, a(x)=cosx, so y=(cosx)y. This single algebraic step replaces an "infinite" object with an ordinary implicit equation.
Step 2: Take the natural logarithm of both sides
logy=ylog(cosx)
This is necessary because y sits in the exponent — logarithmic differentiation is the standard tool whenever the differentiation variable appears as an exponent.
Step 3: Differentiate implicitly with respect to x
The left side needs the chain rule; the right side is a product, so needs the product rule, and log(cosx) itself needs the chain rule: …
Common Mistakes
Mistake 1: Trying to differentiate the infinite tower "layer by layer"
Some students see the infinite exponent tower and attempt to peel off one layer of cosx at a time, which never terminates. Why it's wrong: an infinite tower can't be differentiated term-by-term — it must first be collapsed using its self-referential property. Correct approach: recognize that because the tower repeats forever, the whole tower equals y=(cosx)y, replacing the infinite expression with one clean implicit equation.
Mistake 2: Ignoring the domain/convergence condition
Students often don't pause to note that log(cosx) requires cosx>0, and that the infinite tower only converges for a restricted range of values. Why it's wrong: proceeding without this in mind can mask where the final formula is actually valid. Correct approach: note that the derivation assumes cosx>0 so log(cosx) is defined.
Mistake 3: Sign error differentiating log(cosx), or dropping the product rule on ylog(cosx) …
Showing the 12 most recent of 50 on this concept.
- AP EAPCET 2021Set eng-2021-10-05-FN1 markMCQQ.If yyy⋅⋅⋅∞=log{x+log{x+⋯}}, then dxdy at x=e2−2, y=2 equals _____ (A) 22(e2−1)log2 (B) 22(e2−1)1−log2 (C) e2−12(1−log2) (D) 2(e2−1)log2
›Reveal solutionSolution
Both sides define the same implicit quantity u via a self-referential equation; differentiate each side's defining equation implicitly and combine using the chain rule. The answer is (B).
Concept and Intuition
The infinite power tower yyy⋯=u satisfies the self-consistency equation u=yu (the tower "regenerates" itself). Likewise the infinite nested logarithm log{x+log{x+⋯}}=u satisfies u=log(x+u). Since the problem states these two quantities are equal (both equal to the same u), u is implicitly a common function linking x and y; differentiating each defining relation gives du/dy and du/dx, and the chain rule combines them into dy/dx.
Step-by-Step Solution
- Verify u=2 at the given point. Nested log: u=log(x+u) at x=e2−2: try u=2: log(e2−2+2)=log(e2)=2 ✓. Tower: u=yu at y=2: try u=2: (2)2=2 ✓. Both consistent with u=2.
- Differentiate the tower relation u=yu w.r.t. y. Take log: logu=ulogy. Differentiate: u1dydu=dydulogy+yu ⇒(u1−logy)dydu=yu⇒dydu=y(1−ulogy)u2. At y=2, u=2: dydu=2(1−2log2)4=2(1−ln2)4=1−ln222. …
- AP EAPCET 2021Set eng-2021-08-25-FN1 markMCQQ.If y=x+x+x+⋯∞, then dxdy= (A) y1 (B) x1 (C) 2x−11 (D) 2y−11
›Reveal solutionSolution
The infinite nested radical satisfies y2=x+y (self-similarity), which is then differentiated implicitly.
Concept and Intuition
An infinitely repeating nested expression under a radical satisfies a self-referential equation: the whole expression y equals the same structure with x+y under the first radical (since removing the outermost layer just reproduces y again).
Step-by-Step Solution
- y=x+x+x+⋯=x+y (the inner infinite tail is again y).
- Square both sides: y2=x+y.
- Differentiate implicitly with respect to x: 2ydxdy=1+dxdy.
- Collect: dxdy(2y−1)=1⇒dxdy=2y−11. …
- AP EAPCET 2021Set eng-2021-08-24-AN1 markMCQQ.If y=(tanx)sinx, then dxdy= (A) (tanx)sinx{secx+(cosx)(log(tanx))} (B) (sinx)tanx{secx+(cosx)(log(tanx))} (C) (tanx)sinx{secx−(cosx)(log(tanx))} (D) (sinx)tanx{secx−(cosx)(log(tanx))}
›Reveal solutionSolution
Logarithmic differentiation of y=(tanx)sinx gives y′=(tanx)sinx{secx+cosxlog(tanx)}.
Concept and Intuition
Whenever both the base and the exponent are functions of x (here base tanx, exponent sinx), take natural log of both sides first — this converts the power into a product, which is easy to differentiate using the product rule.
Step-by-Step Solution
- y=(tanx)sinx. Take log: logy=sinx⋅log(tanx).
- Differentiate both sides w.r.t. x using the product rule on the right: y1dxdy=cosx⋅log(tanx)+sinx⋅tanx1⋅sec2x.
- Simplify the second term: sinx⋅tanxsec2x=sinx⋅cos2x1⋅sinxcosx=cosx1=secx.
- So y1dxdy=cosxlog(tanx)+secx. …
- AP EAPCET 2025Set eng-2025-05-26-FN1 markMCQQ.If y=(logxsinx)x, then dxdy= (A) y[logcosxxsinx+log(logsinx)+logx1−log(logx)] (B) y[logsinxxcosx−log(logsinx)+logx1+log(logx)] (C) y[logsinxxcotx+log(logsinx)−logx1−log(logx)] (D) y[logsinxxcotx−log(logsinx)+logx1−logx]
›Reveal solutionSolution
This is a logarithmic-differentiation problem with a function-of-a-function base; careful chain-rule bookkeeping on u=logx(sinx) gives option (C).
Concept and Intuition
When both the base and the exponent are functions of x (here the base is itself logx(sinx)), the standard technique is logarithmic differentiation: take ln of both sides to turn the power into a product, then differentiate using the product and chain rules.
Step-by-Step Solution
- Let u=logx(sinx)=lnxlnsinx, so y=ux.
- Take logs: lny=xlnu.
- Differentiate: yy′=lnu+x⋅uu′.
- Compute u′: with u=lnxlnsinx,
u′=(lnx)2cotx⋅lnx−lnsinx⋅x1.
- Then
uu′=(lnx)2cotx⋅lnx−xlnsinx⋅lnsinxlnx=lnsinxcotx−xlnx1.
- So x⋅uu′=lnsinxxcotx−lnx1.
- And lnu=ln(lnsinx)−ln(lnx).
- Combine:
yy′=ln(lnsinx)−ln(lnx)+lnsinxxcotx−lnx1,
so …
- AP EAPCET 2025Set eng-2025-05-26-FN1 markMCQQ.If sinxcosy−cosysinx=0, then dxdy= (A) tanx (B) 1 (C) −1 (D) −cotx
›Reveal solutionSolution
The given relation simplifies to sinx=cosy; implicit differentiation of this simpler relation gives dxdy=−1.
Concept and Intuition
Many implicit-differentiation problems hide a much simpler relation inside a more complicated-looking equation. Recognizing that both sides share a common factor of sinxcosy lets us cancel down to something we can differentiate directly, instead of differentiating the square-root expression term by term.
Step-by-Step Solution
- Start with sinxcosy−cosysinx=0, i.e. sinxcosy=cosysinx.
- Divide both sides by sinxcosy (both taken positive for the relevant domain):
sinxsinx=cosycosy⇒sinx=cosy.
- Squaring, sinx=cosy.
- Differentiate both sides with respect to x: cosx=−sinydxdy. …
- AP EAPCET 2021Set eng-2021-08-19-AN1 markMCQQ.If log(1+x2−x)=y(1+x2), then (1+x2)dxdy+xy= (A) 0 (B) 1 (C) 2 (D) −1
›Reveal solutionSolution
Implicit differentiation of log(1+x2−x)=y1+x2, using (1+x2−x)(1+x2+x)=1, collapses directly to the requested combination. Answer: −1.
Concept and Intuition
Writing s=1+x2 turns the relation into log(s−x)=ys, a compact form whose derivative — after using the identity s2−x2=1 — telescopes into exactly the expression (1+x2)y′+xy asked for.
Step-by-Step Solution
- Let s=1+x2; then s′=sx and s2−x2=1⇒(s−x)(s+x)=1⇒s−x1=s+x.
- Given: log(s−x)=ys. Differentiate both sides w.r.t. x: s−xs′−1=y′s+ys′ …
- AP EAPCET 2026Set eng-2026-05-12-FN1 markMCQQ.If tan(e3x)=cot(e2y), then at x=0, dxdy= (A) 2−π3 (B) 32−π (C) π−23 (D) 3π−2
›Reveal solutionSolution
Rewrite cot as a shifted tan to turn the equation into an algebraic (exponential) relation between x and y, then implicitly differentiate and evaluate at x=0. Answer: 2−π3.
Concept and Intuition
tanθ1=tanθ2 implies θ1=θ2+nπ for integer n; taking n=0 (the principal relation intended here) converts the trig equation into a clean equation between the exponential expressions, which we can differentiate implicitly.
Step-by-Step Solution
- Use the identity cotθ=tan(2π−θ) with θ=e2y: cot(e2y)=tan(2π−e2y).
- Given tan(e3x)=cot(e2y)=tan(2π−e2y), equate arguments (principal branch): e3x=2π−e2y.
- Rearrange: e3x+e2y=2π.
- Differentiate both sides w.r.t. x: 3e3x+2e2ydxdy=0.
- Solve: dxdy=−2e2y3e3x.
- At x=0: e3x=e0=1. From step 3, 1+e2y=2π⇒e2y=2π−1=2π−2. …
- AP EAPCET 2021Set eng-2021-08-23-AN1 markMCQQ.If y=logyx, then dxdy= ______ (A) xlogy1 (B) x(1+logy)logy (C) x(1+logy)1 (D) 1+logy1
›Reveal solutionSolution
Rewriting y=logyx as ylny=lnx and differentiating implicitly gives dxdy=x(1+logy)1.
Concept and Intuition
logyx means "logarithm of x to base y", i.e. lnylnx. So the given relation y=logyx really means y=lnylnx, or equivalently ylny=lnx — a cleaner form to differentiate implicitly, since it avoids a quotient with y in both places.
Step-by-Step Solution
- y=logyx=lnylnx⇒ylny=lnx.
- Differentiate both sides with respect to x, treating y as a function of x:
dxd(ylny)=dxd(lnx)
- LHS (product rule): dxdylny+y⋅y1dxdy=dxdy(lny+1).
- RHS: x1.
- So dxdy(lny+1)=x1⇒dxdy=x(1+lny)1=x(1+logy)1. …
- AP EAPCET 2022Set eng-2022-07-06-FN1 markMCQQ.If xycos4α+yxsin4α=2sin2α⋅cos2α, then dxdy= (A) sin3αcosα (B) sin2αcos2α (C) cos2αsin2α (D) sinαcos3α
›Reveal solutionSolution
The given relation is secretly a perfect square in disguise; it forces y=xtan2α, so dy/dx=tan2α.
Concept and Intuition
Rather than differentiating implicitly right away, it pays to recognise the algebraic structure first. Multiplying by xy converts the equation into a quadratic in x and y that factors as a perfect square, revealing y/x is actually a constant (independent of x), which makes the derivative trivial.
Step-by-Step Solution
- Start from xycos4α+yxsin4α=2sin2αcos2α.
- Multiply both sides by xy: y2cos4α+x2sin4α=2xysin2αcos2α.
- Rearrange: y2cos4α−2xysin2αcos2α+x2sin4α=0.
- This is (ycos2α−xsin2α)2=0, so ycos2α=xsin2α, i.e. y=xtan2α. …
- AP EAPCET 2025Set eng-2025-05-21-AN1 markMCQQ.If x2+y2=t−t1 and x4+y4=t2+t21, then dxdy= (A) xy (B) x2y2 (C) xy (D) −xy
›Reveal solutionSolution
Eliminating the parameter t between the two given equations produces the direct relation x2y2=−1 between x and y, whose implicit derivative is −y/x.
Concept and Intuition
When x and y are both linked to a parameter t through two equations, differentiating each with respect to t separately (and dividing) works, but it is often faster — and here it is exact — to first eliminate t algebraically to get a direct x–y relation, then differentiate that implicitly in the ordinary way.
Step-by-Step Solution
- Square the first equation: (x2+y2)2=(t−t1)2=t2−2+t21, i.e. x4+2x2y2+y4=t2+t21−2.
- The second equation says x4+y4=t2+t21. Substitute this in: (t2+t21)+2x2y2=t2+t21−2.
- This forces 2x2y2=−2⇒x2y2=−1 — a t-free relation directly linking x and y. …
- AP EAPCET 2026Set eng-2026-05-13-FN1 markMCQQ.If Tan−1x2+Tan−1y2=2π, then (dxdy)(−1,2)= (A) 0 (B) 1 (C) 21 (D) −21
›Reveal solutionSolution
Reducing to y2=x−2 gives dxdy=−x3y1, which at (−1,2) equals 21.
Concept and Intuition
If Tan−1a+Tan−1b=2π with a,b>0, then Tan−1b=2π−Tan−1a=Cot−1a, so b=a1. Applying this to a=x2, b=y2 collapses the relation into an algebraic one.
Step-by-Step Solution
- From Tan−1x2+Tan−1y2=2π we get y2=x21=x−2.
- Differentiate: 2ydxdy=−2x−3.
- Hence dxdy=−x3y1. …
- AP EAPCET 2025Set eng-2025-05-22-AN1 markMCQQ.If x−xy+y−xy=1, then dxdy= (A) −x−x2y−y2 (B) −1−x21−y2 (C) −1−x1−y (D) −x+yx−y
›Reveal solutionSolution
Squaring the constraint reveals that it forces x+y=1 identically, so dxdy=−1 throughout; matching this against the options singles out −x−x2y−y2, since it equals −1 for every point satisfying y=1−x.
Concept and Intuition
Rather than blindly grinding through implicit differentiation of two square roots, it pays to first understand the curve itself. Squaring x−xy+y−xy=1 carefully (using s=x+y,p=xy) collapses to a perfect square equalling zero, revealing that the relation is nothing but the straight line x+y=1. Once we know that, dxdy=−1 is immediate, and we just need to find which option reduces to −1 on this line.
Step-by-Step Solution
- Square the given equation:
x(1−y)+y(1−x)+2xy(1−x)(1−y)=1
x+y−2xy+2xy(1−x)(1−y)=1
- Let s=x+y, p=xy. Then:
2p(1−x)(1−y)=1−s+2p
Note (1−x)(1−y)=1−s+p. Squaring again:
4p(1−s+p)=(1−s+2p)2
Let q=1−s. Expanding both sides: LHS =4pq+4p2; RHS =q2+4pq+4p2. So 0=q2, i.e. q=0, i.e. s=1.
3. Hence x+y=1 is forced — the given relation is the line y=1−x (restricted to the domain where the square roots are real, 0≤x,y≤1).
4. Differentiating y=1−x directly: dxdy=−1.
5. Check which option gives −1 identically along y=1−x:
- (A): y−y2=y(1−y). Substituting y=1−x: y(1−y)=(1−x)⋅x=x−x2. So the ratio is exactly 1, and −1=−1 for every x. ✓ …
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