Q.∫sin2xcos2xsin2x−cos2xdx is equal to (A) tanx+cotx+C (B) tanx+cosecx+C (C) −tanx+cotx+C (D) tanx+secx+C
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Trigonometric Simplification
You know sin2x+cos2x=1 — but the skill of turning a messy trig expression into that kind of clean form is trigonometric simplification. Because sines, cosines and their relatives are all tied together by identities from the unit circle, a tangled combination can almost always be rewritten as something shorter: a single term, a constant, or an easier combination.
Your core toolkit
Pythagorean: sin2θ+cos2θ=1,1+tan2θ=sec2θ,1+cot2θ=csc2θ
Reciprocal: cscθ=sinθ1, secθ=cosθ1, cotθ=tanθ1
Quotient: tanθ=cosθsinθ,cotθ=sinθcosθ
How the process feels
Simplify 1+cosxsinx+sinx1+cosx. Over a common denominator the numerator is sin2x+(1+cosx)2=sin2x+1+2cosx+cos2x. The Pythagorean identity turns sin2x+cos2x into 1, giving 2+2cosx=2(1+cosx), so
sinx(1+cosx)2(1+cosx)=sinx2=2cscx.
A two-term sum collapses to one term.
Strategies that usually work
- Convert everything to sines and cosines — cancellations then appear.
- Spot Pythagorean pairs and replace them with 1 (or sec2, csc2).
- Factor and cancel as you would with ordinary algebra.
- Multiply by a conjugate — e.g. multiply 1+sinx1 by 1−sinx1−sinx to unlock a Pythagorean identity. …
Concept: Trigonometric Simplification — rewrite the numerator using sin2x−cos2x=−(cos2x−sin2x)=−cos2x, but splitting term-by-term is faster.
Step 1: Separate the fraction:
sin2xcos2xsin2x−cos2x=sin2xcos2xsin2x−sin2xcos2xcos2x=cos2x1−sin2x1.
Step 2: Integrate term by term: …
The key idea is to split the integrand into two simpler fractions using the identity sin2x−cos2x=−(cos2x−sin2x)=−cos2x, but an even faster approach is to separate term-by-term: sin2xcos2xsin2x−sin2xcos2xcos2x=sec2x−csc2x. Integrating gives tanx+cotx+C, which matches option (A).
The problem looks like a trigonometric integral, but the real trick is noticing that the denominator is a product of squares. Many students try to use double-angle identities immediately, but the cleanest path is to split the fraction first.
When you have a sum (or difference) in the numerator and a product in the denominator, always check if you can break it into separate terms. Here:
sin2xcos2xsin2x−cos2x=sin2xcos2xsin2x−sin2xcos2xcos2x
Each fraction simplifies beautifully:
sin2xcos2xsin2x=cos2x1=sec2x
sin2xcos2xcos2x=sin2x1=csc2x
So the integrand becomes sec2x−csc2x.
Now integrate term by term:
- ∫sec2xdx=tanx+C1 — this is a standard result, since the derivative of tanx is sec2x.
- ∫csc2xdx=−cotx+C2 — because the derivative of cotx is −csc2x. …
Method: Split sin2xcos2xsin2x−cos2x into sec2 and csc2
When a difference of squared trig terms sits over their product, divide each numerator term by the whole denominator — each piece becomes a standard sec2 or csc2.
Steps
Step 1: Split the fraction.
sin2xcos2xsin2x−cos2x=sin2xcos2xsin2x−sin2xcos2xcos2x
Step 2: Cancel to standard forms.
=cos2x1−sin2x1=sec2x−csc2x
Step 3: Integrate. …
Common Mistakes
Mistake 1: Sign confusion giving −tanx+cotx (option C) instead of tanx+cotx.
Why it's wrong: the fraction splits as sec2x−csc2x; integrating gives tanx−(−cotx)=tanx+cotx, because ∫csc2x=−cotx and there is a leading minus. Correct approach: track both signs carefully to land on option (A).
Mistake 2: Not splitting the numerator and trying a direct substitution. …
Showing the 12 most recent of 34 on this concept.
- TG EAPCET 2023Set eng-2023-05-12-FN1 markMCQQ.If tany=cot(4π−x) then dxdy= (A) 1+cot2(4π+x)csc2(4π−x) (B) sec2y−csc2(4π−x) (C) 1+tan2(4π−x)csc2(4π−x) (D) 1+tan2(4π+x)sec2(4π+x)
›Reveal solutionSolution
Differentiate tany=cot(4π−x) implicitly: sec2ydxdy=csc2(4π−x). Since csc2(4π−x)=sec2(4π+x)=sec2y, the derivative is 1, and option (D) is the form equal to 1.
- Simplify the relation. Using cotθ=tan(2π−θ),
cot(4π−x)=tan(2π−4π+x)=tan(4π+x),
so tany=tan(4π+x), i.e. y=4π+x+nπ and sec2y=sec2(4π+x).
- Differentiate implicitly. With u=4π−x, u′=−1:
sec2ydxdy=−csc2(4π−x)⋅(−1)=csc2(4π−x).
- Convert with a cofunction identity. Because sin(4π−x)=cos(4π+x),
csc2(4π−x)=sec2(4π+x).
Therefore …
- TG EAPCET 2026Set eng-2026-05-10-AN1 markMCQQ.If x=sin−1(cost) and y=tan−1(cost), then dxdy= (A) 1+sin2xcosx (B) 1+sin2tcost (C) 1+sin2tsint (D) 1+cos2xsinx
›Reveal solutionSolution
The key is to express both x and y in terms of t, then use the chain rule to find dxdy as a function of x, matching option (A).
We are given:
x=sin−1(cost),y=tan−1(cost).
We need dxdy.
Concept and intuition:
Both x and y are functions of t, so we can compute dtdy and dtdx separately, then use dxdy=dx/dtdy/dt. The trick is to simplify sin−1(cost) into a nicer algebraic form in terms of t, which will make differentiation cleaner. Then we express the final answer in terms of x (since the options involve x or t).
- Simplify x Recall: sin−1(cost)=2π−t for t in [0,π], but more generally we can use the identity sin−1(cost)=2π−∣t∣? Actually, a cleaner approach: Let u=cost. Then x=sin−1(u). But we can also write cost=sin(2π−t), so
x=sin−1(sin(2π−t)).
For the principal range of sin−1, we need 2π−t∈[−π/2,π/2], i.e., t∈[0,π]. Assuming this, we get
x=2π−t.
Hence, t=2π−x.
- Differentiate x and y with respect to t From x=2π−t, we have
dtdx=−1.
For y=tan−1(cost), differentiate:
dtdy=1+(cost)21⋅(−sint)=−1+cos2tsint.
- Find dxdy Using the chain rule: dxdy=dx/dtdy/dt=−1−1+cos2tsint=1+cos2tsint. …
- TG EAPCET 2023Set eng-2023-05-14-FN1 markMCQQ.If x=log(y+y2+1) then y= (A) tanhx (B) cothx (C) sinhx (D) coshx
›Reveal solutionSolution
The expression x=log(y+y2+1) is the definition of the inverse hyperbolic sine, so y=sinhx. The correct option is (C).
The key here is recognizing a standard identity. The expression y+y2+1 looks like something that appears when you solve for y in terms of x from the definition of hyperbolic sine. In fact, sinhx=2ex−e−x, and its inverse is exactly sinh−1y=log(y+y2+1). So the problem is simply asking: if x=sinh−1y, what is y? The answer is y=sinhx.
Let’s verify this step by step.
-
Start with the given equation
We have x=log(y+y2+1). This is an equation relating x and y. Our goal is to solve for y in terms of x.
-
Exponentiate both sides
Since the logarithm is natural log (base e), we write
ex=y+y2+1.
This removes the log and gives a simpler equation.
- Consider the conjugate expression A classic trick: if ex=y+y2+1, then its reciprocal is
e−x=y+y2+11.
Rationalize the denominator:
e−x=(y+y2+1)(y−y2+1)y−y2+1=y2−(y2+1)y−y2+1=−1y−y2+1=y2+1−y.
So we have two equations:
ex=y+y2+1,e−x=y2+1−y.
- Subtract to isolate y Subtract the second equation from the first:
-
- TG EAPCET 2026Set eng-2026-05-10-FN1 markMCQQ.If y=sin−1(1+sin4x1−cos2x) then dxdy= (A) 1+sin4x2cos2x (B) 1+sin4x2sin2x (C) 1+sin8x2cos2x (D) 1+sin8x2sin2x
›Reveal solutionSolution
The key is to simplify the argument of the inverse sine using trigonometric identities before differentiating. After simplification, the derivative becomes 1+sin4x2sin2x, which matches option (B).
We start with
y=sin−1(1+sin4x1−cos2x).
Concept and intuition
The expression inside the inverse sine looks messy, but the numerator 1−cos2x is a classic form that simplifies to 2sin2x. That’s a huge clue: the whole fraction might simplify to something like 1+sin4x2sin2x, which is a perfect candidate for the identity sin−1(1+t22t)=2tan−1t (for ∣t∣≤1). That substitution makes differentiation straightforward.
Step-by-step
- Simplify the numerator Using the double-angle identity:
1−cos2x=2sin2x.
So the argument becomes
1+sin4x2sin2x.
- Recognize a standard form Let t=sin2x. Then the argument is
1+t22t.
This is exactly the form 1+t22t, which appears in the identity
sin−1(1+t22t)=2tan−1tfor ∣t∣≤1.
Since t=sin2x∈[0,1], the condition holds. Therefore
y=2tan−1(sin2x).
- Differentiate Differentiate y=2tan−1(sin2x):
dxdy=2⋅1+(sin2x)21⋅dxd(sin2x).
The derivative of sin2x is 2sinxcosx=sin2x. So …
- TG EAPCET 2022Set eng-2022-07-18-FN1 markMCQQ.If x=cscθ−sinθ, y=csc2022θ−sin2022θ and (dxdy)2=g(x)k(y2+4) where k∈R, then 10+k−g(2022)= (A) 0 (B) 6 (C) 10 (D) 14
›Reveal solutionSolution
Using cscθ⋅sinθ=1 one gets the standard identity (dxdy)2=x2+4n2(y2+4) with n=2022, so k=20222 and g(x)=x2+4; then 10+k−g(2022)=6, option (B).
Write c=cscθ and s=sinθ, noting the key relation cs=cscθsinθ=1.
Setting up x2+4 and y2+4. With x=c−s and n=2022, y=cn−sn:
x2+4=(c−s)2+4=c2+s2−2cs+4=c2+s2+2=(c+s)2,
y2+4=(cn−sn)2+4=c2n+s2n−2(cs)n+4=c2n+s2n+2=(cn+sn)2,
where cs=1 was used so 2cs=2 and (cs)n=1.
The derivative. Differentiating with respect to θ and forming dxdy=dx/dθdy/dθ, the algebra collapses to the compact identity
(dxdy)2=x2+4n2(y2+4). …
- TG EAPCET 2021Set eng-2021-08-04-AN1 markMCQQ.limx→03x+cosx−3xcosx−1x22x−x2sinx−x2= (A) log31(log2−1) (B) log34(1−log2) (C) log34(log2−1) (D) log32(log2−1)
›Reveal solutionSolution
Factor the denominator as (1−cosx)(3x−1) and expand the numerator to leading order x3(log2−1); the limit is log32(log2−1) — option (D).
Factor the denominator.
3x+cosx−3xcosx−1=3x(1−cosx)−(1−cosx)=(1−cosx)(3x−1).
As x→0: 1−cosx∼2x2 and 3x−1∼xlog3, so the denominator ∼2x3log3.
Expand the numerator x2(2x−sinx−1), using 2x=1+xlog2+O(x2) and sinx=x+O(x3): …
- TG EAPCET 2021Set eng-2021-08-04-AN1 markMCQQ.limx→0xtan2x+32xtan3x(1−cos2x)= (A) −6 (B) 21 (C) 0 (D) 5−6
›Reveal solutionSolution
This problem involves evaluating a limit that results in an indeterminate form 0/0. We resolve this by using the trigonometric identity 1−cos2x=2sin2x and then applying standard limits for sinx/x and tanx/x as x→0. The final value of the limit is 21.
When evaluating limits, the first step is always to try direct substitution. If this yields a finite number, that's your limit. However, if it results in an indeterminate form like 0/0 or ∞/∞, it means the function's behavior near that point is not immediately obvious, and further manipulation is required. For expressions involving trigonometric functions as x→0, we often rely on a set of fundamental limits.
The core idea here is to transform the given expression into a form where these standard limits can be directly applied. This usually involves using trigonometric identities to simplify terms and then dividing the numerator and denominator by appropriate powers of x to create terms like kxsinkx or kxtankx, which approach 1 as x→0.
Let's break down the solution step-by-step.
-
Check for Indeterminate Form
First, substitute x=0 into the expression:
Numerator: 1−cos(2⋅0)=1−cos(0)=1−1=0.
Denominator: 0⋅tan(2⋅0)+32⋅0tan(3⋅0)=0⋅tan(0)+0⋅tan(0)=0⋅0+0⋅0=0.
Since we get the form 00, the limit is indeterminate, and we need to simplify the expression.
-
Apply Trigonometric Identity
The term 1−cos2x in the numerator is a common form that can be simplified using the double-angle identity for cosine: cos2x=1−2sin2x.
Rearranging this, we get:
1−cos2x=2sin2x.
Substituting this into the limit expression:
limx→0xtan2x+32xtan3x2sin2x
- Prepare for Standard Limits
We know the standard limits:
limx→0xsinx=1
limx→0xtanx=1
To use these, we need to divide the numerator and denominator by an appropriate power of x.
The numerator has sin2x, which suggests dividing by x2. The denominator has terms like xtan2x and xtan3x. If we divide by x2, these become xtan2x and xtan3x, which are suitable for the standard limit form.
So, divide both the numerator and the denominator by x2:
limx→0x2xtan2x+32xtan3xx22sin2x
limx→0xtan2x+32xtan3x2(xsinx)2
- Manipulate Terms to Match Standard Forms Now, let's adjust the terms in the denominator to perfectly match the standard limit form kxtankx: For xtan2x, multiply and divide by 2: xtan2x=xtan2x⋅22=2(2xtan2x) …
-
- TG EAPCET 2025Set eng-2025-05-04-FN1 markMCQQ.limx→0sin2xcosx−3cosx= (A) 32 (B) −61 (C) −121 (D) 21
›Reveal solutionSolution
The limit simplifies by factoring out a common power of cosx and using the series expansions for cosx and (1+u)α; the final value is −121, which corresponds to option (C).
We want
L=limx→0sin2xcosx−3cosx.
Both numerator and denominator vanish as x→0, so this is a 00 form. The key is to rewrite the numerator in terms of a common factor and then use expansions near x=0.
1. Factor out the smallest power of cosx.
Write cosx=(cosx)1/2 and 3cosx=(cosx)1/3. The smaller exponent is 31, so factor (cosx)1/3 out:
(cosx)1/2−(cosx)1/3=(cosx)1/3[(cosx)1/6−1].
Thus
L=limx→0sin2x(cosx)1/3[(cosx)1/6−1].
As x→0, cosx→1, so (cosx)1/3→1. That factor is harmless; the interesting part is the bracket.
2. Expand cosx near 0.
We know
cosx=1−2x2+24x4+O(x6).
Also sin2x=x2−3x4+O(x6).
3. Expand (cosx)1/6 using (1+u)α.
Let u=cosx−1=−2x2+24x4+⋯. Then
(cosx)1/6=(1+u)1/6=1+61u+2(1/6)(1/6−1)u2+⋯
=1+61(−2x2+24x4)+61(−65)21(−2x2)2+O(x6).
Compute term by term:
- Linear in u: 61(−2x2)=−12x2, and the 24x4 part gives +144x4.
- Quadratic in u: 61⋅(−65)⋅21=−725, times u2=(−2x2)2=4x4, gives −725⋅4x4=−2885x4.
So
(cosx)1/6−1=−12x2+(1441−2885)x4+O(x6).
The x4 coefficient: 1441=2882, so 2882−2885=−2883=−961.
Thus
(cosx)1/6−1=−12x2−96x4+O(x6).
4. Assemble the limit. …
- TG EAPCET 2022Set eng-2022-07-19-FN1 markMCQQ.If the minimum value of cos(sinh(logx)+cosh(logx)) is k, then cosh(k+1)= (A) 2e+e−1 (B) 2e2+e−2 (C) e (D) 1
›Reveal solutionSolution
The expression simplifies using hyperbolic identities to cos(x+1/x), whose minimum is −1, so k=−1, and cosh(k+1)=cosh0=1.
The problem looks messy at first — cos(sinh(logx)+cosh(logx)) — but the key is to notice that sinh and cosh are built to combine neatly. Their sum is simply elogx, which is x. That turns the whole thing into cos(x+1/x), and then it's just a matter of finding the minimum of a cosine function.
Let's go step by step.
-
Simplify the hyperbolic sum.
Recall the definitions:
sinht=2et−e−t, cosht=2et+e−t.
Adding them:
sinht+cosht=2et−e−t+et+e−t=22et=et.
Here t=logx, so sinh(logx)+cosh(logx)=elogx=x.
-
Rewrite the original expression. …
-
- TG EAPCET 2021Set eng-2021-08-06-AN1 markMCQQ.If θ is the acute angle between the curves x2+y2=20202 and x2−y2=2020, then
[!FORMULA] tanθsinθ+cosθ=
(A) 2 (B) 23+3 (C) 43+3 (D) 63+3›Reveal solutionSolution
The curves cut at 45∘, so tanθsinθ+cosθ=12=2.
Slopes at a point of intersection.
Circle x2+y2=20202: 2x+2yy′=0⇒m1=−yx.
Hyperbola x2−y2=2020: 2x−2yy′=0⇒m2=yx.
tanθ=1+m1m2m1−m2=1−x2/y2−2x/y=y2−x2−2xy.
Point of intersection. Subtracting the equations, 2y2=2020(2−1) and 2x2=2020(2+1), so
y2−x2=1010[(2−1)−(2+1)]=−2020,
x2y2=10102(2+1)(2−1)=10102⇒∣xy∣=1010.
Hence …
- TG EAPCET 2022Set eng-2022-07-19-AN1 markMCQQ.If e1 is the eccentricity of the hyperbola x=secθ,y=2tanθ and e2 is the eccentricity of the hyperbola x=2secθ,y=tanθ, then e12e22= (A) 1 (B) 2 (C) 21 (D) 41
›Reveal solutionSolution
The key idea is to convert each parametric form to its standard Cartesian equation, then use the formula e2=1+a2b2 for hyperbolas. The ratio e12e22 simplifies to 2.
We are given two hyperbolas in parametric form. The first step is always to eliminate the parameter θ to get the standard Cartesian equation. For a hyperbola, the standard forms are a2x2−b2y2=1 (transverse axis along x) or a2y2−b2x2=1 (transverse axis along y). The eccentricity e is then given by e2=1+a2b2 when the transverse axis is along x, and e2=1+b2a2 when it is along y — but the formula e2=1+a2b2 works if we always take a as the denominator under the positive term. We'll be careful.
- First hyperbola: x=secθ, y=2tanθ. Recall the identity sec2θ−tan2θ=1. Here x=secθ and 2y=tanθ. Substituting into the identity:
x2−(2y)2=1⇒x2−2y2=1.
This is 12x2−(2)2y2=1, so a12=1, b12=2. The transverse axis is along x. Hence
e12=1+a12b12=1+12=3.
- Second hyperbola: x=2secθ, y=tanθ. Here 2x=secθ and y=tanθ. Using the same identity: (2x)2−y2=1⇒2x2−y2=1. …
- TG EAPCET 2025Set eng-2025-05-02-FN1 markMCQQ.tan−153+tan−1416+tan−11919= (A) tan−1109 (B) tan−11918 (C) tan−11913 (D) tan−12056
›Reveal solutionSolution
Adding the arctangents two at a time gives tan−1109.
Solution
Use tan−1p+tan−1q=tan−11−pqp+q.
First two terms:
tan−153+tan−1416=tan−11−53⋅41653+416=tan−1205−18123+30=tan−1187153=tan−1119.
Add the third term: …
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