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 17 on this concept.
- TG EAPCET 2024Set eng-2024-05-11-FN1 markMCQQ.Derivative of (sinx)x with respect to x(sinx) is (A) x(sinx)[xcosx(logx)+sinx](sinx)x−1[(sinx)log(sinx)+xcosx] (B) x(sinx)[xcosx(logx)+sinx](sinx)x[(sinx)(log(sinx))+xcosx] (C) (sinx)x−1[(sinx)log(sinx)+xcosx]xsinx−1[xcosx(logx)+sinx] (D) (sinx)x[(sinx)log(sinx)+xcosx]xsinx[xcosx(logx)+sinx]
›Reveal solutionSolution
Differentiate both u=(sinx)x and v=xsinx logarithmically, then form dv/dxdu/dx. The numerator is (sinx)x−1[sinxlog(sinx)+xcosx] and the denominator carries [xcosxlogx+sinx] — option (A).
The concept first. Two ideas combine.
- Derivative of one function w.r.t. another. By the chain rule, dvdu=dv/dxdu/dx. So we never need to eliminate x; we just differentiate each separately and divide.
- Logarithmic differentiation. Neither the power rule (xn, constant exponent) nor the exponential rule (ax, constant base) applies when both base and exponent depend on x. Taking log first turns the exponent into a product, which the product rule can handle.
Step 1 — Differentiate u=(sinx)x.
logu=xlog(sinx)
Differentiate both sides:
u1dxdu=log(sinx)+x⋅sinxcosx
dxdu=(sinx)x[log(sinx)+sinxxcosx]=(sinx)x−1[sinxlog(sinx)+xcosx]
(the last step just takes one factor of sinx out of the bracket).
Step 2 — Differentiate v=xsinx.
logv=sinxlogx
v1dxdv=cosxlogx+xsinx
dxdv=xsinx[cosxlogx+xsinx]=xsinx⋅x1[xcosxlogx+sinx]
Step 3 — Divide. …
- TG EAPCET 2024Set eng-2024-05-11-FN1 markMCQQ.A function f:R→R is such that yf(x+y)+cosmy=1+yf(x). If m=2, then f′(x)= (A) −2sin2xy (B) 4x (C) y2sin2xy (D) 2x2
›Reveal solutionSolution
Rearranging the relation gives yf(x+y)−f(x)=y21−cos(mxy); letting y→0 and using 1−cosθ→θ2/2 yields f′(x)=2m2x2=2x2 for m=2 — option (D).
The concept first. The derivative is defined by
f′(x)=limy→0yf(x+y)−f(x)
So whenever a problem hands you a relation connecting f(x+y) and f(x), the strategy is always the same: isolate f(x+y)−f(x), divide by y, and take the limit. The answer must be a function of x alone — y is the vanishing increment, so any option still containing y (like (A) and (C)) cannot be a derivative at all.
Step 1 — Isolate the difference.
yf(x+y)+cos(mxy)=1+yf(x)
⇒yf(x+y)−yf(x)=1−cos(mxy)
⇒y[f(x+y)−f(x)]=1−cos(mxy)
Step 2 — Build the difference quotient. Divide both sides by y2 (valid for y=0):
yf(x+y)−f(x)=y21−cos(mxy)
Step 3 — Take the limit y→0.
Use the standard limit 1−cosθ=2sin2(2θ), so for small θ, 1−cosθ≈2θ2. With θ=mxy: …
- TG EAPCET 2021Set eng-2021-08-04-AN1 markMCQQ.If (a+bx)exy=x, then dx2d2y= (A) x31(xy′+y2)2 (B) x31(xy′+y2) (C) x31(xy′−y) (D) x31(xy′−y)2
›Reveal solutionSolution
By simplifying the given equation using logarithms and then applying implicit differentiation twice, we find that the second derivative dx2d2y is x31(xy′−y)2.
The problem asks us to find the second derivative dx2d2y from the given implicit relation (a+bx)exy=x. The presence of the exponential term exy suggests that taking the natural logarithm might simplify the expression, making differentiation easier. The options provided involve the term (xy′−y), which is a strong hint that we should try to express our derivatives in terms of this quantity.
Here's a step-by-step approach:
-
Simplify the given equation:
The initial equation is (a+bx)exy=x.
To simplify, first isolate the exponential term:
exy=a+bxx
Now, take the natural logarithm on both sides. This brings the exponent down, making the equation linear in xy:
log(exy)=log(a+bxx)
Using the logarithm property log(A/B)=logA−logB:
xy=logx−log(a+bx)
Multiplying by x gives us an explicit expression for y:
y=x(logx−log(a+bx))
-
Find the first derivative, y′:
We differentiate y=x(logx−log(a+bx)) with respect to x. We will use the product rule, (uv)′=u′v+uv′.
Let u=x, so u′=1.
Let v=logx−log(a+bx). To find v′, we differentiate term by term:
dxd(logx)=x1
dxd(log(a+bx))=a+bx1⋅dxd(a+bx)=a+bxb
So, v′=x1−a+bxb.
Applying the product rule for y′:
y′=(1)⋅(logx−log(a+bx))+x⋅(x1−a+bxb)
y′=(logx−log(a+bx))+1−a+bxbx
From Step 1, we know that logx−log(a+bx)=xy. Substitute this back into the expression for y′:
y′=xy+1−a+bxbx
Combine the constant and fractional terms:
y′=xy+a+bx(a+bx)−bx
y′=xy+a+bxa
-
Express xy′−y:
The options involve the term (xy′−y). Let's rearrange our expression for y′ from Step 2 to find this:
y′−xy=a+bxa
Multiply the entire equation by x:
x(y′−xy)=x(a+bxa)
xy′−y=a+bxax
This is a key intermediate result.
-
Find the second derivative, y′′:
Now we differentiate y′=xy+a+bxa with respect to x to find y′′.
y′′=dxd(xy)+dxd(a+bxa)
For the first term, dxd(xy), use the quotient rule (vu)′=v2u′v−uv′:
dxd(xy)=x2y′⋅x−y⋅1=x2xy′−y
For the second term, dxd(a+bxa), treat it as a(a+bx)−1 and use the chain rule:
dxd(a(a+bx)−1)=a⋅(−1)(a+bx)−2⋅dxd(a+bx)
=−a(a+bx)−2⋅b=−(a+bx)2ab
Combining these, we get y′′: …
-
- TG EAPCET 2025Set eng-2025-05-03-AN1 markMCQQ.If x=sin2θcos3θ, y=sin3θcos2θ, then dxdy= (A) 2cos5θ−cos3θcos2θ2cos5θ+sin3θsin2θ (B) 2cos5θ+cos3θcos2θ2cos5θ−sin3θsin2θ (C) 2cos5θ−sin3θsin2θ2cos5θ+cos3θcos2θ (D) 2cos5θ−cos3θcos2θ2cos5θ−sin3θsin2θ
›Reveal solutionSolution
dxdy=2cos5θ−sin3θsin2θ2cos5θ+cos3θcos2θ.
Differentiate each with respect to θ:
dθdx=2cos2θcos3θ−3sin2θsin3θ,
dθdy=3cos3θcos2θ−2sin3θsin2θ.
Using cos5θ=cos2θcos3θ−sin2θsin3θ, write each derivative around cos5θ:
dθdx=2(cos2θcos3θ−sin2θsin3θ)−sin3θsin2θ=2cos5θ−sin3θsin2θ, …
- TG EAPCET 2025Set eng-2025-05-03-FN1 markMCQQ.If x=sin2θcos3θ, y=sin3θcos2θ, then dxdy= (A) 2cos5θ−sin3θsin2θ2cos5θ+cos3θcos2θ (B) 2cos5θ+cos3θcos2θ2cos5θ+sin3θsin2θ (C) 2cos5θ+cos3θcos2θ2cos5θ−sin3θsin2θ (D) 2cos5θ−sin3θsin2θ2cos5θ−cos3θcos2θ
›Reveal solutionSolution
Parametric differentiation gives dxdy=2cos5θ−sin3θsin2θ2cos5θ+cos3θcos2θ. Option (A).
Solution
With x=sin2θcos3θ and y=sin3θcos2θ, differentiate each by the product rule:
dθdx=2cos2θcos3θ−3sin2θsin3θ,dθdy=3cos3θcos2θ−2sin3θsin2θ.
Use cos5θ=cos(3θ+2θ)=cos3θcos2θ−sin3θsin2θ, i.e.
2cos5θ=2cos3θcos2θ−2sin3θsin2θ.
Numerator:
dθdy=(2cos3θcos2θ−2sin3θsin2θ)+cos3θcos2θ=2cos5θ+cos3θcos2θ.
Denominator: …
- TG EAPCET 2024Set eng-2024-05-10-FN1 markMCQQ.If y=acos3x+be−x, then y′′(3sin3x−cos3x)= (A) 10y′sin3x+3y(sin3x+3cos3x) (B) 10y′cos3x+3y(sin3x+3cos3x) (C) 10y′cos3x+3y(cos3x+3sin3x) (D) 10y′cos3x+3y(sin3x−3cos3x)
›Reveal solutionSolution
The key idea is to compute the first and second derivatives of y=acos3x+be−x, then substitute into the expression y′′(3sin3x−cos3x) and simplify to match one of the given forms. The result simplifies to 10y′cos3x+3y(sin3x+3cos3x), which corresponds to option (B).
We start with the given function:
y=acos3x+be−x
We need to find an expression for y′′(3sin3x−cos3x) in terms of y and y′. The trick is to avoid solving for a and b explicitly — instead, we differentiate and then cleverly combine terms.
1. Compute the first derivative y′
Differentiate term by term:
y′=−3asin3x−be−x
(Recall: derivative of cos3x is −3sin3x, and derivative of e−x is −e−x.)
2. Compute the second derivative y′′
Differentiate y′:
y′′=−9acos3x+be−x
(Derivative of −3asin3x is −9acos3x; derivative of −be−x is +be−x because −e−x differentiates to e−x.)
3. Form the expression y′′(3sin3x−cos3x)
Substitute y′′:
y′′(3sin3x−cos3x)=(−9acos3x+be−x)(3sin3x−cos3x)
Expand:
=−27acos3xsin3x+9acos23x+3be−xsin3x−be−xcos3x
4. Express everything in terms of y and y′
We have:
y=acos3x+be−x
y′=−3asin3x−be−x
We want to rewrite the expanded expression. Notice the terms:
- 9acos23x can be linked to y and y′ if we also have sin2 terms, but we don't. Instead, we aim to match the pattern in the options, which involve y′cos3x and y(sin3x+3cos3x).
5. Try to express acos3x and be−x from y and y′
From y and y′ we can solve:
y=acos3x+be−x
y′=−3asin3x−be−x
Add them:
y+y′=acos3x−3asin3x=a(cos3x−3sin3x)
So:
a=cos3x−3sin3xy+y′
Also subtract:
y−y′=acos3x+3asin3x+2be−x
But this gets messy. Instead, a better approach: directly compute the target expression using derivatives and compare to options.
6. Compute y′′ in terms of y and y′
Notice that from y′=−3asin3x−be−x, we can differentiate again but also note:
y′′=−9acos3x+be−x
We can write y′′ as a combination of y and y′:
y=acos3x+be−x
y′=−3asin3x−be−x
Multiply y by something and y′ by something to get y′′. Try:
y′′=−9acos3x+be−x=αy+βy′
Substitute:
α(acos3x+be−x)+β(−3asin3x−be−x)=a(αcos3x−3βsin3x)+be−x(α−β)
Compare with y′′=−9acos3x+be−x:
- Coefficient of acos3x: α=−9
- Coefficient of asin3x: −3β=0⇒β=0
- Coefficient of be−x: α−β=−9=1? That gives −9=1, impossible.
So y′′ is not a linear combination of y and y′ alone (because the sine and cosine terms have different dependencies). So we must work directly.
7. Instead, compute y′′(3sin3x−cos3x) by substituting y′′ and then replace acos3x and be−x using y and y′
We have:
y′′(3sin3x−cos3x)=(−9acos3x+be−x)(3sin3x−cos3x)
Expand:
=−27acos3xsin3x+9acos23x+3be−xsin3x−be−xcos3x
Now, note that y′=−3asin3x−be−x, so 3asin3x=−y′−be−x. But we have −27acos3xsin3x=−9cos3x(3asin3x)=−9cos3x(−y′−be−x)=9y′cos3x+9be−xcos3x.
So the expression becomes:
=9y′cos3x+9be−xcos3x+9acos23x+3be−xsin3x−be−xcos3x
Combine the be−xcos3x terms: 9be−xcos3x−be−xcos3x=8be−xcos3x.
So:
=9y′cos3x+9acos23x+3be−xsin3x+8be−xcos3x
8. Now rewrite 9acos23x
We know y=acos3x+be−x, so acos3x=y−be−x. Then:
9acos23x=9cos3x(acos3x)=9cos3x(y−be−x)=9ycos3x−9be−xcos3x
Substitute back:
=9y′cos3x+(9ycos3x−9be−xcos3x)+3be−xsin3x+8be−xcos3x
Combine the be−xcos3x: −9+8=−1, so we get −be−xcos3x.
Thus:
=9y′cos3x+9ycos3x+3be−xsin3x−be−xcos3x
9. Factor be−x terms
Notice 3be−xsin3x−be−xcos3x=be−x(3sin3x−cos3x). But be−x=y−acos3x. However, we can also write be−x=y−acos3x, but we want everything in y and y′. Alternatively, note that y′=−3asin3x−be−x doesn't directly give be−x alone.
Instead, observe that 3ysin3x=3acos3xsin3x+3be−xsin3x. And 9ycos3x we already have. Let's try to match the options: they all have 10y′cos3x+3y(something).
10. Compare with option (B): 10y′cos3x+3y(sin3x+3cos3x)
Expand option (B):
10y′cos3x+3ysin3x+9ycos3x
Our expression is:
9y′cos3x+9ycos3x+3be−xsin3x−be−xcos3x
We need to turn 9y′cos3x into 10y′cos3x and the remaining terms into 3ysin3x. That suggests y′cos3x appears with coefficient 10, so we might have missed a y′cos3x term. Let's re-check step 7: we had 9y′cos3x from the manipulation, but perhaps there's an extra y′cos3x hidden.
11. Alternative direct substitution
Let’s compute y′′(3sin3x−cos3x) by writing y′′ in terms of y and y′ using the original differential equation. Since y=acos3x+be−x, note that y satisfies a linear ODE. Differentiate twice: y′=−3asin3x−be−x, y′′=−9acos3x+be−x. Add 9y:
y′′+9y=(−9acos3x+be−x)+9(acos3x+be−x)=10be−x …
- TG EAPCET 2026Set eng-2026-05-10-FN1 markMCQQ.The differential equation corresponding to the family of curves y=loge(ax+3), where a is an arbitrary constant is (A) xdxdy+3e−x=1 (B) xdxdy+3ey=1 (C) xdxdy+3e−y=1 (D) xdxdy+3ex=1
›Reveal solutionSolution
The key idea is to eliminate the arbitrary constant a by differentiating the given family and then substituting back. The correct differential equation is xdxdy+3e−y=1, which corresponds to option (C).
We are given a family of curves y=loge(ax+3), where a is an arbitrary constant. To find its differential equation, we need an equation involving x, y, and dxdy that holds for every curve in the family — meaning a must be eliminated.
The natural approach: differentiate the given relation, then use the original equation to replace a in terms of x and y.
- Differentiate both sides with respect to x. Since y=ln(ax+3), we have
dxdy=ax+3a.
- Express a from the original equation. From y=ln(ax+3), exponentiate:
ey=ax+3⇒ax=ey−3⇒a=xey−3.
- Substitute a into the derivative. Replace a in dxdy=ax+3a:
dxdy=eyxey−3=xeyey−3.
- Rearrange to match the given options. Multiply both sides by xey:
xeydxdy=ey−3.
Bring terms together:
xeydxdy−ey=−3.
Factor ey:
ey(xdxdy−1)=−3. …
- TG EAPCET 2021Set eng-2021-08-04-AN1 markMCQQ.The equation of the tangent to the curve y=πe−x/π at the point where it crosses Y-axis is (A) πx+2y=2π (B) 2x+πy=π2 (C) x−y+π=0 (D) x+y=π
›Reveal solutionSolution
To find the tangent's equation, first locate the point where the curve crosses the Y-axis, then calculate the curve's derivative at that point to get the tangent's slope. Finally, use the point-slope form. The equation of the tangent is x+y=π.
The equation of a straight line, such as a tangent, can be determined if we know two things: a point it passes through and its slope. For a tangent line to a curve, the point it passes through is the point of tangency on the curve itself. The slope of the tangent at that specific point is given by the value of the derivative of the curve's equation at that point.
Here's how we find the equation of the tangent:
-
Identify the point of tangency:
The problem states that the tangent is at the point where the curve y=πe−x/π crosses the Y-axis. A curve crosses the Y-axis when its x-coordinate is 0.
Substitute x=0 into the curve's equation:
y=πe−0/π
y=πe0
Since e0=1, we have:
y=π×1=π
So, the point of tangency is (0,π).
-
Calculate the slope of the tangent:
The slope of the tangent at any point (x,y) on the curve is given by the derivative dxdy.
The curve's equation is y=πe−x/π.
Differentiate y with respect to x using the chain rule: dxd(ef(x))=ef(x)⋅f′(x).
Here, f(x)=−πx, so f′(x)=−π1.
dxdy=π⋅dxd(e−x/π)
dxdy=π⋅e−x/π⋅(−π1)
dxdy=−e−x/π
Now, evaluate the derivative at the point of tangency, where x=0:
m=dxdyx=0=−e−0/π=−e0=−1
The slope of the tangent at (0,π) is −1. …
-
- TG EAPCET 2023Set eng-2023-05-12-FN1 markMCQQ.If x=32cos3θ and y=4tan2θ then (dxdy)θ=π/4= (A) 9322 (B) 916 (C) −916 (D) −932
›Reveal solutionSolution
With x=32cos3θ, y=4tan2θ, the parametric derivative reduces to dxdy=92cos5θ−8; at θ=4π this is −932, option (D).
- Differentiate each parameter.
dθdx=32⋅3cos2θ⋅(−sinθ)=−92cos2θsinθ,
dθdy=4⋅2tanθsec2θ=8tanθsec2θ.
- Form the ratio.
dxdy=−92cos2θsinθ8tanθsec2θ.
Since tanθsec2θ=cos3θsinθ,
dxdy=−92cos2θsinθ8cos3θsinθ=92cos5θ−8. …
- TG EAPCET 2023Set eng-2023-05-13-AN1 markMCQQ.If x=cos3θ−sin3θ and y=3cosθ−3sinθ, then the value of dxdy at θ=4π is (A) 9232 (B) 332 (C) 9432 (D) 932
›Reveal solutionSolution
Differentiate x and y separately with respect to the parameter θ and divide. At θ=π/4 this gives dxdy=94⋅2−2/3=9232 — option (A).
The concept first
When both coordinates are given through a parameter, x=x(θ) and y=y(θ), the chain rule gives
dxdy=dx/dθdy/dθ(provided dθdx=0).
Never try to eliminate θ here — with a cube and a cube root in the same problem that would be brutal. Just differentiate each expression in θ and take the quotient at the required value.
The symmetry sin4π=cos4π=21 makes the arithmetic collapse very neatly, so keep the powers of 2 in index form until the end.
Step-by-step
- Differentiate x=cos3θ−sin3θ:
dθdx=3cos2θ(−sinθ)−3sin2θ(cosθ)=−3sinθcosθ(cosθ+sinθ).
- Differentiate y=cos1/3θ−sin1/3θ:
dθdy=31cos−2/3θ(−sinθ)−31sin−2/3θ(cosθ)=−31(sinθcos−2/3θ+cosθsin−2/3θ).
- Put θ=4π, where sinθ=cosθ=2−1/2: dθdx=−3(21)(22)=−3⋅21⋅2=−232. …
- TG EAPCET 2021Set eng-2021-08-06-AN1 markMCQQ.The differential equation for which y2=4a(x+a) (where a is a parameter) is general solution, is (A) y−yy′2=2xy′ (B) y+yy′2=2xy′ (C) y(y+y′)=2xy′ (D) y(y−y′)=2xy′
›Reveal solutionSolution
To find the differential equation, we eliminate the arbitrary parameter a from the given general solution y2=4a(x+a) by differentiating it once. The resulting differential equation is y−yy′2=2xy′.
When we are given a general solution to a differential equation, it contains one or more arbitrary constants (parameters). The process of finding the differential equation involves eliminating these arbitrary constants. The number of times we need to differentiate the given solution is equal to the number of independent arbitrary constants present in it.
In this problem, the general solution is y2=4a(x+a), and a is the single arbitrary parameter. Therefore, we will differentiate the equation once with respect to x to obtain an expression involving a, and then substitute this expression back into the original equation to eliminate a.
Here's the step-by-step derivation:
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Identify the arbitrary parameter:
The given general solution is y2=4a(x+a).
Here, a is the only arbitrary parameter. Since there is one arbitrary parameter, the differential equation will be of the first order, meaning we will need to differentiate the given equation once with respect to x.
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Differentiate the equation with respect to x:
We differentiate both sides of y2=4a(x+a) with respect to x. Remember to use the chain rule for y2 and treat a as a constant.
dxd(y2)=dxd(4a(x+a))
2ydxdy=4adxd(x+a)
2yy′=4a(1+0)
2yy′=4a
From this, we can express $a$ in terms of $y$ and $y'$:a=42yy′
a=2yy′
- Eliminate the parameter a: Now, substitute the expression for a back into the original general solution y2=4a(x+a). y2=4(2yy′)(x+2yy′) …
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- TG EAPCET 2021Set eng-2021-08-04-FN1 markMCQQ.If x2+xy+y2=k, then dx2d2y= (A) (x+2y)3−6k (B) (x+2y)2−6k (C) (2x+y)2x2+xy+y2 (D) 0
›Reveal solutionSolution
Implicit differentiation twice gives dx2d2y=(x+2y)3−6k — option (A).
Step 1 — First derivative. Differentiate x2+xy+y2=k:
2x+y+xy′+2yy′=0⇒y′=−x+2y2x+y.
Step 2 — Second derivative. With y′=−vu where u=2x+y, v=x+2y (so u′=2+y′, v′=1+2y′):
y′′=−v2u′v−uv′.
Compute the numerator:
u′v−uv′=(2+y′)(x+2y)−(2x+y)(1+2y′)=3y−3xy′.
Substitute y′=−x+2y2x+y: …
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