Q.If π(π₯) = π₯ tanβ1 π₯ , then πβ²(1)is equal to
(A) π 4 β 1 2
(B) π 4 + 1 2
(C) β π 4 β 1 2
(D) β π 4 + 1 2
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Derivative Evaluation
To evaluate a derivative means to find fβ²(a) β a single number that tells you how fast f is changing right at x=a. Think of a speedometer: it doesn't report how far you've travelled, only how fast your position is changing at this instant. That instantaneous rate of change is exactly what fβ²(a) measures.
The geometric picture
On the curve y=f(x), pick a point P and a nearby point Q. The straight line through them β the secant β has slope equal to the average rate of change between P and Q. Now slide Q toward P: the secant rotates into the tangent line that just touches the curve at P, and its slope is fβ²(a).
fβ²(a) is the slope of the tangent to y=f(x) at x=a β how steep the curve is right there.
The limit definition
fβ²(a)=limhβ0βhf(a+h)βf(a)β
Here h is a tiny step from a to a+h, the numerator is the matching change in height, and the ratio is a secant slope. As hβ0 the secant becomes the tangent. An equivalent form is
fβ²(a)=limxβaβxβaf(x)βf(a)β.
When this limit exists, f is differentiable at a (which forces continuity there).
Continuity alone is not enough. f(x)=β£xβ£ is continuous at 0, but its left slope β1 and right slope +1 disagree, so fβ²(0) does not exist β a corner has no single tangent.
A worked evaluation
For f(x)=x2 at x=3:
fβ²(3)=limhβ0βh(3+h)2β9β=limhβ0β(6+h)=6.
So the tangent at x=3 has slope 6.
From a number to a function β¦
Concept: Derivative Evaluation β differentiate f(x)=xtanβ1x using the product rule, then substitute x=1.
Step 1: Apply product rule:
fβ²(x)=(1)β tanβ1x+xβ 1+x21β.
Step 2: Simplify:
fβ²(x)=tanβ1x+1+x2xβ.
Step 3: Substitute x=1: β¦
The derivative of f(x)=xtanβ1x is found using the product rule. Evaluating at x=1 gives fβ²(1)=4Οβ+21β, which corresponds to option (B).
The key here is recognizing that f(x) is a product of two functions: x and tanβ1x (inverse tangent, also written as arctanx). When you see a product, your first instinct should be the product rule β not expanding or simplifying, because thereβs nothing to simplify here. The derivative of tanβ1x is a standard result: dxdβtanβ1x=1+x21β. Thatβs the only βtrickyβ part; everything else is straightforward algebra.
Letβs walk through it.
-
Apply the product rule.
For f(x)=u(x)β v(x), we have fβ²(x)=uβ²(x)v(x)+u(x)vβ²(x).
Here, let u(x)=x and v(x)=tanβ1x.
Then uβ²(x)=1, and vβ²(x)=1+x21β.
So:
fβ²(x)=(1)β tanβ1x+xβ 1+x21β=tanβ1x+1+x2xβ.
- Evaluate at x=1. Substitute x=1 into the derivative:
fβ²(1)=tanβ1(1)+1+121β=tanβ1(1)+21β.
Now, tanβ1(1) is the angle whose tangent is 1. That angle is 4Οβ (since tan4Οβ=1).
Therefore:
fβ²(1)=4Οβ+21β.
- Match with the options. The options are given as combinations of 4Οβ and 21β with plus/minus signs. Our result 4Οβ+21β exactly matches option (B). β¦
Method: Differentiating a Product Involving an Inverse Trigonometric Function
Use this method whenever f(x) is a product of a simple algebraic factor (like x) and an inverse trig function (like tanβ1x, sinβ1x, etc.), and you need fβ²(a) at a specific point.
Steps
Step 1: Recognize the product structure
Identify the two factors being multiplied, u(x) and v(x), so you know to reach for the product rule rather than trying to simplify the expression first (there is usually nothing to simplify before differentiating).
Step 2: Recall the standard derivative of the inverse trig factor
Memorize (or quickly re-derive) the standard results:
dxdβtanβ1x=1+x21β,dxdβsinβ1x=1βx2β1β,dxdβcosβ1x=1βx2ββ1β. β¦
Common Mistakes
Mistake 1: Skipping the product rule
A student might try to differentiate xtanβ1x as if it were a single function, or differentiate only the tanβ1x part and ignore the leading x. Why it's wrong: whenever two functions of x are multiplied together, both factors contribute to the derivative through the product rule; dropping one term silently loses information. Correct approach: explicitly label u(x)=x and v(x)=tanβ1x before differentiating, so both terms are accounted for.
Mistake 2: Confusing the derivative of tanβ1x with the derivative of tanx β¦
Showing the 12 most recent of 50 on this concept.
- TG EAPCET 2025Set eng-2025-05-02-FN1 markMCQQ.If f(x)=cosβ11βx2ββ, then fβ²(21β)= (A) Ο2ββ (B) 2Οββ (C) βΟ2ββ (D) β2Οββ
βΊReveal solutionSolution
For xβ₯0, cosβ11βx2β=sinβ1x, so f(x)=sinβ1xβ and fβ²(21β)=Ο2ββ β option (A).
Simplify. For 0β€xβ€1, let ΞΈ=cosβ11βx2ββ[0,2Οβ]. Then cos2ΞΈ=1βx2, so sinΞΈ=x and ΞΈ=sinβ1x. Hence
f(x)=sinβ1xβ.
Differentiate.
fβ²(x)=2sinβ1xβ1ββ 1βx2β1β.
Evaluate at x=21β. sinβ121β=6Οβ and 1β41ββ=23ββ: β¦
- TG EAPCET 2024Set eng-2024-05-10-AN1 markMCQQ.If β«(cscx+1β)dx=ktanβ1(f(x))+c, then k1βf(6Οβ)= (A) 21β (B) 41β (C) β41β (D) β21β
βΊReveal solutionSolution
β«cscx+1βdx=β2tanβ1(cscxβ1β)+c, so k=β2, f(x)=cscxβ1β and k1βf(6Οβ)=β21β.
Evaluating the integral.
Write cscx+1β=sinx1+sinxββ. We claim
β«cscx+1βdx=β2tanβ1(cscxβ1β)+c.
Verification by differentiation.
Let g=cscxβ1β, so g2=cscxβ1 and 1+g2=cscx. Then
2ggβ²=βcscxcotxβgβ²=2gβcscxcotxβ.
dxdβ[β2tanβ1g]=1+g2β2gβ²β=cscxβ2gβ²β=gcotxβ=sinxsinx1βsinxββcosxβ=sinxβ1βsinxβcosxβ.
Since cosx=1βsin2xβ=1βsinxβ1+sinxβ, this reduces to β¦
- TG EAPCET 2026Set eng-2026-05-09-FN1 markMCQQ.If dxdyβ=(x3βx)β(1β3x2)tanx+(x3βx)tan2x and y(1)=0, then Ο64βy(4Οβ)= (A) 1 (B) Ο2+16 (C) Ο2β16 (D) 16Ο2
βΊReveal solutionSolution
The key is to notice that the derivative simplifies to a perfect derivative of a product involving tanx and a polynomial, so we can integrate directly and then evaluate at x=Ο/4. The final value is Ο2β16, which corresponds to option (C).
We are given:
dxdyβ=(x3βx)β(1β3x2)tanx+(x3βx)tan2x
with y(1)=0, and we need Ο64βy(Ο/4).
Concept and intuition:
The expression looks messy, but the presence of tanx and tan2x alongside a polynomial suggests it might be the derivative of something like (polynomial)β tanx plus something simpler. When we differentiate a product u(x)tanx, we get uβ²(x)tanx+u(x)sec2x. Since sec2x=1+tan2x, this can produce terms like u(x)+u(x)tan2x plus a uβ²(x)tanx term. That matches our structure perfectly.
Letβs try to match it.
- Guess the form Suppose y(x)=(x3βx)tanx+something. Differentiate:
dxdβ[(x3βx)tanx]=(3x2β1)tanx+(x3βx)sec2x.
Since sec2x=1+tan2x, this becomes:
(3x2β1)tanx+(x3βx)+(x3βx)tan2x.
- Compare with given dxdyβ The given derivative is:
(x3βx)β(1β3x2)tanx+(x3βx)tan2x.
Notice that β(1β3x2)=3x2β1. So the given derivative is exactly:
(x3βx)+(3x2β1)tanx+(x3βx)tan2x.
This matches the derivative we computed for (x3βx)tanx term by term.
- Conclusion about y(x) Hence,
dxdyβ=dxdβ[(x3βx)tanx].
Integrating both sides:
y(x)=(x3βx)tanx+C.
- Use the initial condition y(1)=0 gives:
0=(13β1)tan1+C=0β tan1+C=C.
So C=0, and
y(x)=(x3βx)tanx.
- Evaluate at x=Ο/4
- TG EAPCET 2022Set eng-2022-07-19-AN1 markMCQQ.If x=logeβ(cot(4Οβ+ΞΈ)), then limΞΈβ0β(sinhx)(coshx)ΞΈβ= (A) 0 (B) β21β (C) β2 (D) 1
βΊReveal solutionSolution
The key idea is to simplify x using log properties and trig identities, then rewrite the limit in terms of ΞΈ using hyperbolic function definitions. The limit evaluates to β21β, so option (B) is correct.
We start with the given expression:
x=logeβ(cot(4Οβ+ΞΈ)).
The goal is to find limΞΈβ0β(sinhx)(coshx)ΞΈβ.
The presence of sinhx and coshx suggests we should first simplify x itself. The argument of the log involves a cotangent of a sum, which often simplifies using trigonometric identities. Once x is expressed in terms of ΞΈ, the hyperbolic functions become manageable, and the limit reduces to a standard form.
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Simplify x using a trig identity.
Recall that cot(4Οβ+ΞΈ)=1+tanΞΈ1βtanΞΈβ.
This comes from cot(A+B)=cotA+cotBcotAcotBβ1β, but a quicker route:
cot(4Οβ+ΞΈ)=sin(4Οβ+ΞΈ)cos(4Οβ+ΞΈ)β, and using cos(4Οβ+ΞΈ)=2β1β(cosΞΈβsinΞΈ), sin(4Οβ+ΞΈ)=2β1β(cosΞΈ+sinΞΈ), the ratio gives cosΞΈ+sinΞΈcosΞΈβsinΞΈβ=1+tanΞΈ1βtanΞΈβ.
So x=logeβ(1+tanΞΈ1βtanΞΈβ).
-
Rewrite x using log properties.
x=logeβ(1βtanΞΈ)βlogeβ(1+tanΞΈ).
For small ΞΈ, tanΞΈβΞΈ, so we can expand:
logeβ(1βΞΈ)ββΞΈβ2ΞΈ2βββ― and logeβ(1+ΞΈ)βΞΈβ2ΞΈ2β+β―.
Thus xβ(βΞΈβ2ΞΈ2β)β(ΞΈβ2ΞΈ2β)=β2ΞΈ, ignoring higher-order terms.
More precisely, x=β2ΞΈ+O(ΞΈ3) as ΞΈβ0.
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Express sinhx and coshx in terms of ΞΈ.
For small x, sinhxβx and coshxβ1+2x2β.
But here xββ2ΞΈ, so sinhxββ2ΞΈ and coshxβ1+2(β2ΞΈ)2β=1+2ΞΈ2.
Therefore (sinhx)(coshx)β(β2ΞΈ)(1+2ΞΈ2)=β2ΞΈβ4ΞΈ3.
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Form the limit expression.
(sinhx)(coshx)ΞΈβββ2ΞΈβ4ΞΈ3ΞΈβ=β2β4ΞΈ21β. β¦
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- TG EAPCET 2023Set eng-2023-05-12-AN1 markMCQQ.limnβββ[n21βsec2n1β+n22βsec2n2β+n24βsec2n4β+β¦+n1βsec21]= (A) 21βsec(1) (B) 21βcosec(1) (C) tan(1) (D) 21βtan(1)
βΊReveal solutionSolution
The sum is a Riemann sum for β«01βxsec2(x2)dx=21βtan1.
Identify the Riemann sum. The general term is
tkβ=n2kβsec2n2k2β=n1ββ nkβsec2(nkβ)2,
and the last term (k=n) is n2nβsec2n2n2β=n1βsec21, matching the final entry. Writing xkβ=nkβ with spacing Ξx=n1β,
βk=1nβtkβ=βk=1nβn1βf(nkβ),f(x)=xsec2(x2).
Take the limit as an integral. β¦
- TG EAPCET 2022Set eng-2022-07-18-AN1 markMCQQ.If tanhx=21β then sinh2xβsech2x= (A) 1529β (B) 1511β (C) 3 (D) 15β13β
βΊReveal solutionSolution
Use the given tanhx=21β to find sinh2x and \sech2x via hyperbolic identities, then subtract to get 1529β.
The core idea here is that hyperbolic functions obey identities very similar to trigonometric ones, but with sign differences. Given tanhx, you can find sinhx and coshx using the fundamental relation cosh2xβsinh2x=1, then compute double-angle forms. The trick is to avoid solving for x directly β work algebraically with the ratios.
- Find coshx and sinhx from tanhx. Let tanhx=coshxsinhxβ=21β. So sinhx=21βcoshx. Use cosh2xβsinh2x=1:
cosh2xβ(21βcoshx)2=1βcosh2xβ41βcosh2x=43βcosh2x=1.
Hence cosh2x=34β, so coshx=3β2β (positive, since coshx>0 for all real x).
Then sinhx=21ββ 3β2β=3β1β.
- Compute sinh2x. Using sinh2x=2sinhxcoshx:
sinh2x=2β 3β1ββ 3β2β=34β.
- Compute cosh2x and then \sech2x. Use cosh2x=cosh2x+sinh2x (note: plus sign, unlike cos2x):
- TG EAPCET 2021Set eng-2021-08-04-FN1 markMCQQ.If the tangent at a point P on the curve y=4x4+x is perpendicular to the tangent to the same curve at (0, 0), then the point P is (A) (2β1β,4β1β) (B) (21β,43β) (C) (1,5) (D) (β1,3)
βΊReveal solutionSolution
To find the point P, we first determine the slope of the tangent at (0, 0) using the derivative. Since the tangent at P is perpendicular to this, its slope must be the negative reciprocal. We then set the general derivative equal to this required slope to find the x-coordinate of P, and finally use the curve equation to find the y-coordinate. The point P is (2β1β,4β1β)β.
The slope of the tangent to a curve at any point is given by the derivative of the curve's equation with respect to x, evaluated at that point. This derivative, dxdyβ, represents the instantaneous rate of change of y with respect to x, which is precisely the slope of the line tangent to the curve.
For two lines to be perpendicular, the product of their slopes must be β1. If one line has a slope m1β and the other has a slope m2β, then m1ββ m2β=β1. This condition is key to solving the problem.
Here's how we apply these concepts:
- Find the derivative of the curve: The given curve is y=4x4+x. We differentiate y with respect to x to find the general expression for the slope of the tangent at any point (x,y):
dxdyβ=dxdβ(4x4+x)=16x3+1
- Calculate the slope of the tangent at (0, 0): Let m1β be the slope of the tangent at the point (0,0). We substitute x=0 into the derivative:
m1β=dxdyββx=0β=16(0)3+1=1
- Determine the required slope for the tangent at point P:
Let m2β be the slope of the tangent at point P. We are given that the tangent at P is perpendicular to the tangent at (0, 0).
For two perpendicular lines with slopes m1β and m2β, we have m1ββ m2β=β1.
Using this condition:
1β m2β=β1
m2β=β1
So, the tangent at point P must have a slope of $-1$.4. Find the x-coordinate of point P:
We know that the slope of the tangent at any point (x,y) is 16x3+1. We set this equal to the required slope m2β=β1:
16x3+1=β1
16x3=β2
x3=16β2β
$$ x^3 = \frac{-1}{8} $$ β¦ - TG EAPCET 2021Set eng-2021-08-06-FN1 markMCQQ.
[!FORMULA] limxβ0ββx21β(1βcos2x)ββ=
(A) 2β1β (B) 2ββ1β (C) β1 (D) does not existβΊReveal solutionSolution
The key is to simplify the numerator using sin2xβ=β£sinxβ£, then consider the left-hand limit where sinx is negative. The limit equals β2β1β.
The expression involves a square root of a trigonometric square, which always gives a non-negative result. That absolute-value behaviour is the entire crux β the sign of sinx near x=0β decides the answer.
- Simplify the numerator. Recall cos2x=1βsin2x, so
21β(1βcos2x)=21β(1β(1βsin2x))=21βsin2x.
Therefore
21β(1βcos2x)β=21βsin2xβ=2β1ββ£sinxβ£.
- Rewrite the limit. The given limit becomes
limxβ0ββx2β1ββ£sinxβ£β=2β1βlimxβ0ββxβ£sinxβ£β.
- Handle the sign for xβ0β. For x just less than 0, sinx is negative (since sin is odd and positive for small positive x). Hence β£sinxβ£=βsinx. So
xβ£sinxβ£β=xβsinxβ=βxsinxβ.
- Use the standard limit. β¦
- TG EAPCET 2022Set eng-2022-07-19-FN1 markMCQQ.If (x+1)(2x2+3)3x+5β=x+1Aβ+2x2+3Bx+Cβ and f(x)=Ax3+Bx2+7x+C, then 5Cβfβ²(β2)= (A) 19 (B) 15 (C) 4 (D) 34
βΊReveal solutionSolution
We first decompose the given rational function into partial fractions to find the constants A, B, and C. Then, we use these constants to define the polynomial f(x), differentiate it to find fβ²(x), and evaluate fβ²(β2). Finally, we compute the required expression 5Cβfβ²(β2), which evaluates to 4β.
The problem combines two key calculus concepts: partial fraction decomposition and differentiation of polynomials. The core idea is to first determine the unknown constants A, B, and C by equating the given rational function with its partial fraction form. Once these constants are known, we can fully define the polynomial function f(x). The next step involves finding the derivative of f(x), denoted as fβ²(x), and evaluating it at a specific point, x=β2. Finally, we substitute the calculated values into the expression 5Cβfβ²(β2) to arrive at the final answer.
Here's a step-by-step breakdown:
- Determine the constants A, B, and C using partial fraction decomposition. We are given the identity:
(x+1)(2x2+3)3x+5β=x+1Aβ+2x2+3Bx+Cβ
To find $A$, $B$, and $C$, we combine the terms on the right-hand side:(x+1)(2x2+3)A(2x2+3)+(Bx+C)(x+1)β
Equating the numerators from both sides, we get:3x+5=A(2x2+3)+(Bx+C)(x+1)
This equation must hold for all values of $x$. We can find the constants using two methods: * **Method of Substitution (for $A$):** To find $A$, we can choose a value of $x$ that makes the term $(Bx+C)(x+1)$ zero. This happens when $x+1=0$, i.e., $x=-1$. Substitute $x=-1$ into the equation:3(β1)+5=A(2(β1)2+3)+(B(β1)+C)(β1+1)
β3+5=A(2(1)+3)+(CβB)(0)
2=A(2+3)+0
2=5A
A=52β
* **Method of Comparing Coefficients (for $B$ and $C$):** Expand the right side of the equation $3x+5 = A(2x^2+3) + (Bx+C)(x+1)$:3x+5=2Ax2+3A+Bx2+Bx+Cx+C
Group terms by powers of $x$:3x+5=(2A+B)x2+(B+C)x+(3A+C)
Now, compare the coefficients of $x^2$, $x$, and the constant terms on both sides: * **Coefficient of $x^2$:**0=2A+B
Since $A = \frac{2}{5}$:0=2(52β)+B
0=54β+BβΉB=β54β
* **Coefficient of $x$:**3=B+C
Since $B = -\frac{4}{5}$:3=β54β+C
C=3+54β=515+4β=519β
* **Constant term (for verification):**5=3A+C
Substitute $A = \frac{2}{5}$ and $C = \frac{19}{5}$:5=3(52β)+519β
5=56β+519β=525β
5=5
This confirms our values for $A$, $B$, and $C$. So, we have $A = \frac{2}{5}$, $B = -\frac{4}{5}$, and $C = \frac{19}{5}$.2. Define f(x) and find its derivative fβ²(x).
We are given f(x)=Ax3+Bx2+7x+C. β¦
- TG EAPCET 2022Set eng-2022-07-18-AN1 markMCQQ.If β«excosxdx=2exβ(cosx+sinx) and β«(3β2x)2cos(log(3β2x2x+3β))βdx=24f(x)β[cos(g(x))+sin(g(x))]+c then g(1)= (A) 5 (B) logf(2) (C) logf(1) (D) 0
βΊReveal solutionSolution
This problem requires recognizing a pattern in the given integral formula to evaluate a more complex integral. By identifying the correct substitution, the complex integral transforms into the standard form, allowing us to determine g(x) and f(x). We find g(1)=log5, which matches logf(1). The correct option is (C).
The core idea here is to recognize that the second integral's structure is a generalized form of the first integral. The given formula β«excosxdx=2exβ(cosx+sinx) provides a template. When we see the result of the second integral in the form 24f(x)β[cos(g(x))+sin(g(x))], it strongly suggests that g(x) is the argument of the cosine function in the integrand, and f(x) is related to eg(x). Our strategy will be to make a suitable substitution to transform the second integral into the standard form β«etcostdt.
-
Identify the potential g(x):
The argument of the cosine function in the second integral is log(3β2x2x+3β). Given the form of the result, it is highly probable that this expression is g(x).
Let g(x)=log(3β2x2x+3β).
-
Calculate the derivative of g(x):
We can rewrite g(x) using logarithm properties: g(x)=log(2x+3)βlog(3β2x).
Now, differentiate g(x) with respect to x:
gβ²(x)=dxdβ(log(2x+3))βdxdβ(log(3β2x))
gβ²(x)=2x+31ββ (2)β3β2x1ββ (β2)
gβ²(x)=2x+32β+3β2x2β
Combine the terms:
gβ²(x)=2(2x+31β+3β2x1β)
gβ²(x)=2((2x+3)(3β2x)(3β2x)+(2x+3)β)
gβ²(x)=2((2x+3)(3β2x)6β)
gβ²(x)=(2x+3)(3β2x)12β
-
Determine eg(x):
From g(x)=log(3β2x2x+3β), we have:
eg(x)=elog(3β2x2x+3β)=3β2x2x+3β.
-
Relate eg(x)gβ²(x) to the integrand:
Let's multiply eg(x) and gβ²(x):
eg(x)gβ²(x)=(3β2x2x+3β)β ((2x+3)(3β2x)12β)
eg(x)gβ²(x)=(3β2x)212β.
Now, observe the integrand of the second integral: (3β2x)2cos(log(3β2x2x+3β))β.
We can rewrite this using g(x) and the expression for eg(x)gβ²(x):
(3β2x)2cos(g(x))β=cos(g(x))β 121β((3β2x)212β)
(3β2x)2cos(g(x))β=121βcos(g(x))eg(x)gβ²(x).
-
Perform the integration:
The integral becomes:
β«121βeg(x)cos(g(x))gβ²(x)dx
Let t=g(x). Then dt=gβ²(x)dx.
The integral transforms to:
121ββ«etcostdt.
Using the given formula β«excosxdx=2exβ(cosx+sinx): β¦
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- TG EAPCET 2024Set eng-2024-05-10-AN1 markMCQQ.If Rolle's Theorem is applicable for the function f(x)={xplogx,0,βxξ =0x=0β on the interval [0,1], then a possible value of p is (A) β2 (B) β1 (C) 0 (D) 1
βΊReveal solutionSolution
Rolleβs Theorem requires continuity on [0,1] and differentiability on (0,1) with f(0)=f(1). For f(x)=xplogx (with f(0)=0), continuity at 0 forces p>0, so only p=1 works among the options.
The key idea is that Rolleβs Theorem is a threeβpart contract: the function must be continuous on the closed interval, differentiable on the open interval, and take equal values at the endpoints. Here the only tricky part is the behavior at x=0, because logx blows up as xβ0+. The exponent p must be strong enough to tame that blowβup.
-
Check endpoint equality
We have f(1)=1plog1=0, and f(0)=0 by definition. So f(0)=f(1) holds for any p β no restriction yet.
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Continuity on [0,1]
The only potential trouble is at x=0. For x>0, f(x)=xplogx. We need
limxβ0+βxplogx=f(0)=0.
Recall that logxβββ as xβ0+, so xp must go to 0 fast enough to overpower it.
- If p>0, then xpβ0 and xplogxβ0 (a standard limit: xΟ΅logxβ0 for any Ο΅>0).
- If p=0, then f(x)=logxβββ, so the limit is not 0.
- If p<0, then xpβ+β and the product xplogxβββ (or +β depending on sign), so the limit is not 0. Hence continuity at 0 forces p>0.
- Differentiability on (0,1) β¦
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- TG EAPCET 2026Set eng-2026-05-10-FN1 markMCQQ.Approximate volume of a cone whose semi vertical angle is tanβ1(3) and base radius is 15.001 is (A) (375.025)Ο (B) (325.025)Ο (C) (375.075)Ο (D) (325.075)Ο
βΊReveal solutionSolution
With tanΞ±=r/h=3, V=9Οr3β; using dV=3Οr2βdr at r=15,Β dr=0.001 gives Vβ(375.075)Ο.
Semi-vertical angle Ξ±=tanβ1(3), so tanΞ±=hrβ=3βh=3rβ.
V=31βΟr2h=31βΟr2β 3rβ=9Οr3β.
At r=15: V=9Ο(3375)β=375Ο.
Differential for a small change dr=0.001 about r=15: β¦
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