Q.(C) cosβ1(3π₯) (D) 3 cosβ1 π₯ 1 h
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π Start your 14-day free trial to unlock the full solution βConcept understanding β Inverse Secant Domain
Domain of Inverse Secant
To define secβ1x we ask: for which values of x does the equation secΞΈ=x have a solution? The answer is the domain of inverse secant, and it looks quite different from the domain of sinβ1 or cosβ1.
Why β£xβ£β₯1
Recall secΞΈ=cosΞΈ1β, and cosΞΈ always lies in [β1,1]. Taking reciprocals:
- when β£cosΞΈβ£β€1, we get β£secΞΈβ£β₯1.
So secant never outputs a value strictly between β1 and 1. There is simply no angle whose secant is, say, 0.5. Therefore
DomainΒ ofΒ secβ1x:β£xβ£β₯1,i.e.Β (ββ,β1]βͺ[1,β).
The interval (β1,1) is excluded β this is the single most-tested fact about inverse secant.
The matching range
Like every trig function, secant repeats, so we must restrict it to make it one-to-one before inverting. The conventional principal-value choice keeps ΞΈ in
[0,Ο]β{2Οβ}.
We remove ΞΈ=2Οβ because cos2Οβ=0, so sec2Οβ is undefined. On [0,2Οβ) secant runs from 1 up to +β, covering [1,β); on (2Οβ,Ο] it runs from ββ up to β1, covering (ββ,β1]. Together these give exactly β£xβ£β₯1 β matching the domain above. β¦
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Held β figure not available. This is a graph-identification question whose answer depends entirely on the figure printed in the original exam paper, which is not present in our source data. We are honestly holding i β¦
Method: Finding the Domain of Expressions Involving the Inverse Secant Function
Because this specific question's underlying figure/content could not be recovered (its answer is honestly held), this Method tab teaches the general technique for the domain-of-inverse-secant family of problems this concept covers, so it still applies once the question is restored or to any sibling question of the same type.
Steps
Step 1: Isolate the secβ1(β ) sub-expression
Identify exactly what is being fed into secβ1 β it might be a plain variable, or an algebraic expression like secβ1(3x) or secβ1(x1β).
Step 2: Apply the domain restriction for inverse secant
secβ1(u)Β isΒ definedΒ onlyΒ whenΒ β£uβ£β₯1,i.e.Β uβ€β1Β orΒ uβ₯1.
Substitute the actual inner expression for u and write this as an inequality in x.
Step 3: Solve the inequality for x
Solve β£u(x)β£β₯1 using standard inequality techniques, being careful with any sign flips introduced by dividing by a negative quantity. β¦
- TG EAPCET 2025Set eng-2025-05-03-AN1 markMCQQ.If y=secβ1x, then dx2d2yβ= (A) xβ£xβ£(x2β1)23β1β2x2β (B) x2(x2β1)23β1βx2β (C) βx2(x2β1)23β1βx2β (D) xβ£xβ£(x2β1)23β1+2x2β
βΊReveal solutionSolution
The second derivative of secβ1x is found by differentiating the known derivative β£xβ£x2β1β1β using the chain rule and careful handling of the absolute value, leading to the result xβ£xβ£(x2β1)3/21β2x2β, which matches option (A).
We start with the function y=secβ1x. The key idea is to recall the derivative of the inverse secant and then differentiate again, being meticulous about the domain and the absolute value that appears. The absolute value is not just a decorationβit affects the sign of the derivative and must be handled algebraically.
Step-by-step derivation:
- Recall the first derivative. For y=secβ1x, the standard formula is
dxdyβ=β£xβ£x2β1β1β,β£xβ£>1.
The absolute value arises because the range of secβ1x is [0,Ο] excluding Ο/2, and the derivative must be positive for x>1 and also positive for x<β1 (since the function is decreasing there, but the derivative formula with β£xβ£ corrects the sign).
- Rewrite the derivative without the absolute value using a piecewise approach or a clever identity. A useful trick: β£xβ£=x2β, but that can be messy for differentiation. Instead, note that
β£xβ£1β=xβ sgn(x)1β,
but a cleaner method is to write
dxdyβ=xx2β1β1βforΒ x>1,
and
dxdyβ=xx2β1ββ1βforΒ x<β1.
However, we can unify these by observing that
dxdyβ=xx2β1β1βforΒ x>1,
and for x<β1, x is negative, so 1/x is negative, but we need the derivative to be positive. Actually, check: For x<β1, secβ1x is in (Ο/2,Ο], and its derivative is positive. If we used xx2β1β1β, then x negative gives a negative valueβwrong. So the absolute value is essential.
The unified form β£xβ£x2β1β1β is correct for all β£xβ£>1.
- Differentiate again using the chain rule. Let
dxdyβ=(β£xβ£)β1(x2β1)β1/2.
But differentiating β£xβ£ directly is tricky. Instead, write β£xβ£=x2β, so
dxdyβ=x2βx2β1β1β=(x2)β1/2(x2β1)β1/2.
Now differentiate using the product rule:
dx2d2yβ=dxdβ[(x2)β1/2]β (x2β1)β1/2+(x2)β1/2β dxdβ[(x2β1)β1/2].
- Compute each derivative.
- First term:
dxdβ(x2)β1/2=β21β(x2)β3/2β 2x=β(x2)3/2xβ=ββ£xβ£3xβ.
But $(x^2)^{3/2} = |x|^3$, so this is $-\frac{x}{|x|^3}$.- Second term:
dxdβ(x2β1)β1/2=β21β(x2β1)β3/2β 2x=β(x2β1)3/2xβ.
- Assemble the second derivative.
dx2d2yβ=(ββ£xβ£3xβ)β x2β1β1β+β£xβ£1ββ (β(x2β1)3/2xβ).
Factor common terms:
dx2d2yβ=ββ£xβ£xβ[β£xβ£2x2β1β1β+(x2β1)3/21β]. β¦
- TG EAPCET 2024Set eng-2024-05-11-FN1 markMCQQ.Sechβ1(53β)βTanhβ1(53β)= (A) logeβ6 (B) logeβ5 (C) logeβ(23β) (D) logeβ(32β)
βΊReveal solutionSolution
Using the logarithmic forms, Sechβ1(53β)=ln3 and Tanhβ1(53β)=ln2, so the difference is ln(23β), option (C).
Step 1 β Evaluate Sechβ1(53β).
For 0<xβ€1, Β Sechβ1(x)=ln(x1+1βx2ββ). With x=53β:
1β259ββ=2516ββ=54β,Sechβ1(53β)=ln(53β1+54ββ)=ln(3/59/5β)=ln3.
Step 2 β Evaluate Tanhβ1(53β).
For β£xβ£<1, Β Tanhβ1(x)=21βln(1βx1+xβ). With x=53β: β¦
- TG EAPCET 2022Set eng-2022-07-20-FN1 markMCQQ.If sinhx=tanA, then β£tanhxβ£= (A) β£sinAβ£ (B) β£cosAβ£ (C) β£secAβ£ (D) β£cosecAβ£
βΊReveal solutionSolution
The key is to express tanhx in terms of sinhx using the identity tanhx=1+sinh2xβsinhxβ, then substitute sinhx=tanA and simplify to get β£tanhxβ£=β£sinAβ£, so the correct option is (A).
The problem gives sinhx=tanA and asks for β£tanhxβ£ in terms of A. The core idea is to relate hyperbolic functions through their fundamental identity: cosh2xβsinh2x=1. This is the hyperbolic analogue of cos2ΞΈ+sin2ΞΈ=1, and it lets us express tanhx purely in terms of sinhx (or coshx). Once we do that, substituting sinhx=tanA turns the expression into something involving only trigonometric functions of A, which simplifies neatly.
-
Recall the definition of tanhx
tanhx=coshxsinhxβ.
So to find β£tanhxβ£, we need coshx in terms of sinhx.
-
Use the hyperbolic identity
cosh2xβsinh2x=1βcosh2x=1+sinh2x.
Since coshxβ₯1 for all real x, we take the positive square root:
coshx=1+sinh2xβ.
-
Express tanhx
tanhx=1+sinh2xβsinhxβ.
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Substitute the given sinhx=tanA
tanhx=1+tan2AβtanAβ.
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Simplify the denominator using a trigonometric identity
Recall: 1+tan2A=sec2A.
So 1+tan2Aβ=sec2Aβ=β£secAβ£ (the absolute value is needed because secA can be negative, but the square root gives a non-negative result).
-
Write tanhx in terms of A
tanhx=β£secAβ£tanAβ.
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Simplify further β¦
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- TG EAPCET 2021Set eng-2021-08-05-AN1 markMCQQ.Let a>1 be a constant. If f:AβA and (x,y)βf satisfy ax+ay=a, then A= (A) (0,a] (B) [0,a] (C) (ββ,1) (D) (ββ,a+1)
βΊReveal solutionSolution
The condition ax+ay=a forces both x and y to be less than 1, and since a>1, the domain A must be (ββ,1) for the relation to be possible for all pairs in f.
The key idea here is that f is a function from A to A, meaning every x in A pairs with some y in A such that (x,y)βf. The given equation ax+ay=a must hold for these pairs. Since a>1, the exponential at is strictly increasing, and its range is (0,β). We need to find the largest set A such that for every x in A, there exists a y in A satisfying the equation β and vice versa, because f is a relation on AΓA.
Letβs work through the constraints step by step.
-
Rewrite the condition.
From ax+ay=a, we get ay=aβax. Since ay>0 for any real y, we require aβax>0, i.e., ax<a. Because a>1, the exponential function is increasing, so ax<a implies x<1. Similarly, by symmetry, y<1 as well. So both coordinates must be strictly less than 1.
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What about lower bounds?
There is no lower bound from positivity alone: ax can be arbitrarily close to 0 as xβββ, and then ay=aβax approaches a, so y approaches 1 from below. Conversely, if x is very close to 1 from below, ax is just under a, making ay very small, so yβββ. So x and y can each be any real number less than 1, with no minimum.
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Check the endpoints.
Can x=1? Then ax=a, so ay=0, which is impossible because ay>0 for all real y. So 1 is not allowed. Can x be exactly 0? Yes, a0=1, then ay=aβ1>0, so y=logaβ(aβ1), which is a real number less than 1. So 0 is fine. Similarly, any negative number works.
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What about x being greater than 1? β¦
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