Q.Integrate the following function: sin3(2x+1)
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🔒 Start your 14-day free trial to unlock the full solution →Concept understanding — U Substitution
U Substitution: The Reverse Chain Rule
The chain rule differentiates composite functions: the derivative of sin(x2) is cos(x2)⋅2x — differentiate the outer function, then multiply by the derivative of the inside. Integration asks the reverse: given cos(x2)⋅2x, find the original function. That's what u substitution does — it reverses the chain rule.
The Core Intuition
When an integral looks like "a function times the derivative of its inside," substitute the inside with u and the derivative of the inside with du. Consider:
∫2xcos(x2)dx
Here 2x is the derivative of x2, and x2 is the inside of cos(x2). Let u=x2, so du=2xdx:
∫cos(u)du=sin(u)+C=sin(x2)+C
Check: the derivative of sin(x2) is cos(x2)⋅2x.
The Precise Statement
∫f(g(x))⋅g′(x)dx=∫f(u)duwhere u=g(x),du=g′(x)dx
Valid provided g is differentiable and the resulting integral in u is simpler.
The Step-by-Step Method
- Identify a function g(x) whose derivative g′(x) also appears (possibly up to a constant factor).
- Set u=g(x), compute du=g′(x)dx.
- Rewrite the entire integral in u and du — every x and dx must be replaced.
- Integrate with respect to u.
- Substitute back u=g(x).
You cannot mix variables. If any x remains after substitution, you chose the wrong u (or must solve for x in terms of u — rare).
A Second Example (with a constant factor)
Evaluate ∫xx2+1dx. Let u=x2+1, so xdx=21du:
∫u⋅21du=21⋅32u3/2+C=31(x2+1)3/2+C
When Does It Work?
When the integrand is something times the derivative of something inside. Common patterns:
- x⋅f(x2) — derivative of x2 is 2x, so u=x2
- eg(x)⋅g′(x) — derivative of g(x) appears
- g(x)g′(x) — leads to log∣g(x)∣ …
Concept: U Substitution — reduce the odd power using sin2θ=1−cos2θ, then substitute for the cosine.
Step 1: Let u=2x+1, so du=2dx and dx=2du.
The integral becomes
21∫sin3udu.
Step 2: Write sin3u=sinu⋅sin2u=sinu(1−cos2u).
Then
21∫sinu(1−cos2u)du.
Step 3: Substitute t=cosu, dt=−sinudu. The integral becomes …
The key idea is to rewrite sin3(2x+1) as sin(2x+1)⋅sin2(2x+1), then use the identity sin2θ=1−cos2θ to set up a u-substitution with u=cos(2x+1). The final integral is −21cos(2x+1)+61cos3(2x+1)+C.
When you see an odd power of sine (or cosine), your first instinct should be to peel off one factor. Why? Because the remaining even power can be rewritten using the Pythagorean identity, turning the integral into a form ready for substitution.
Here, the function is sin3(2x+1). The argument (2x+1) is linear, so the chain rule will eventually give us a factor of 21 after substitution. Let’s walk through it.
- Separate one sine factor Write sin3(2x+1)=sin(2x+1)⋅sin2(2x+1). This lets us use the identity sin2θ=1−cos2θ on the squared part:
sin3(2x+1)=sin(2x+1)⋅(1−cos2(2x+1)).
-
Choose the substitution
The expression now contains sin(2x+1) and cos(2x+1). If we set u=cos(2x+1), then the derivative is du=−2sin(2x+1)dx.
This is perfect: the sin(2x+1)dx in our integral will be replaced by −21du.
Watch outA common mistake is forgetting the factor of 2 from the chain rule when differentiating cos(2x+1). Always check: derivative of cos(2x+1) is −sin(2x+1)⋅2, so du=−2sin(2x+1)dx.
-
Rewrite the integral
The original integral is
∫sin3(2x+1)dx=∫sin(2x+1)⋅(1−cos2(2x+1))dx.
Substitute u=cos(2x+1) and dx=−2sin(2x+1)du:
∫sin(2x+1)⋅(1−u2)⋅(−2sin(2x+1)du).
The sin(2x+1) cancels neatly, leaving:
∫(1−u2)⋅(−21)du=−21∫(1−u2)du. …
Method: Odd power of sine — save one factor and substitute
When an odd power of sin (of any linear argument) is integrated, peel off one sine factor to pair with dx and convert the rest to cosine, so a u=cos(⋅) substitution works.
Steps
Step 1: Split the odd power, keeping one sine aside.
sin3θ=sin2θ⋅sinθ=(1−cos2θ)sinθ
using sin2θ=1−cos2θ. The lone sinθ is what pairs with the differential.
Step 2: Substitute u=cosθ.
With θ the linear argument (e.g. θ=2x+1),
u=cosθ,du=−sinθ⋅θ′dx
so the spare sinθdx becomes a constant times du. …
Common Mistakes
Mistake 1: Writing ∫sin3(2x+1)dx=4sin4(2x+1).
Why it's wrong: the power rule does not apply to sin3 without a matching cos(2x+1) differential. Correct approach: split sin3θ=(1−cos2θ)sinθ and substitute u=cos(2x+1).
Mistake 2: Forgetting the 21 from du=−2sin(2x+1)dx. …
Showing the 12 most recent of 16 on this concept.
- COMEDK 2021Set 2021-B1 markMCQQ.∫1−cos3xcosx−cos3xdx= (A) −31log1−cos3/2x1+cos3/2x+c (B) −31logcos3/2x+1cos3/2x−1+c (C) −32sin−1(cos3/2x)+c (D) −32sin−1(cos3x)+c
›Reveal solutionSolution
The integral equals −32sin−1(cos3/2x)+c.
Simplify the radicand: cosx−cos3x=cosx(1−cos2x)=cosxsin2x, so
1−cos3xcosx−cos3x=1−cos3xcosx∣sinx∣.
Let u=cos3/2x. Then dxdu=23cos1/2x⋅(−sinx)=−23cosxsinx, so cosxsinxdx=−32du, and 1−cos3x=1−u2.
Thus …
- COMEDK 2024Set 2024-M1 markMCQQ.
[!FORMULA] The value of ∫x+x−11dx is
(A) log(x+x−1)+sin−1(xx−1)+C (B) log(x+x−1)−32tan−1(32x−1+1)+C (C) log(x+x−1)+C (D) log(x−1+x−1)+31logx−2+3x−2−3+C›Reveal solutionSolution
The integral simplifies by substituting t=x−1, turning it into a rational function that integrates to a logarithm and an arctangent, matching option (B).
We are asked to evaluate
∫x+x−11dx.
The presence of x−1 suggests a substitution that removes the square root, turning the integrand into a rational function. The trick is to set t=x−1, so that x=t2+1 and dx=2tdt. This transforms the integral into a form we can handle with partial fractions or a standard arctangent formula.
Let’s work through it step by step.
- Substitute t=x−1. Then x=t2+1 and dx=2tdt. The denominator becomes
x+x−1=(t2+1)+t=t2+t+1.
So the integral becomes
∫t2+t+11⋅2tdt=2∫t2+t+1tdt.
- Prepare for integration by rewriting the numerator to match the derivative of the denominator. The derivative of t2+t+1 is 2t+1. We have 2t in the numerator, so write
2t=(2t+1)−1.
Then
2∫t2+t+1tdt=∫t2+t+12t+1dt−∫t2+t+11dt.
- First integral:
∫t2+t+12t+1dt=log∣t2+t+1∣+C1.
Since t2+t+1>0 for all real t, we can drop the absolute value.
- Second integral: Complete the square in the denominator:
t2+t+1=(t+21)2+43.
So
∫t2+t+11dt=∫(t+21)2+(23)21dt.
Using the formula ∫u2+a2du=a1tan−1(au), with u=t+21 and a=23, we get
∫t2+t+11dt=32tan−1(32t+1)+C2.
- Combine results:
- COMEDK 2023Set 2023-M1 markMCQQ.∫2(1+x)3/2xdx is equal to (A) 1+x2+x+C (B) x1+x2+x+C (C) 1+xx+C (D) −1+xx+C
›Reveal solutionSolution
With u=1+x, the integral becomes 21∫(u−1/2−u−3/2)du=u1/2+u−1/2=1+x2+x+C.
∫2(1+x)3/2xdx. Let u=1+x⇒x=u−1, dx=du:
21∫u3/2u−1du=21∫(u−1/2−u−3/2)du. …
- COMEDK 2022Set 20221 markMCQQ.∫1−9x3xdx is equal to (A) (log3)sin−13x+C (B) 31sin−1(3x)+C (C) log31sin−13x+C (D) 3log3sin−13x+C
›Reveal solutionSolution
I = (1/log 3) * Integral du / sqrt(1 - u^2) = (1/log 3) * arcsin(u) + C = (1 / log 3) * sin^-1 (3^x) + C
Concept: Substitution reducing to the arcsin form, integral du/sqrt(1 - u^2) = arcsin u.
I = Integral of 3^x / sqrt(1 - 9^x) dx , and 9^x = (3^x)^2
Put u = 3^x => du = 3^x (log 3) dx => 3^x dx = du / log 3
I = (1/log 3) * Integral du / sqrt(1 - u^2) …
- COMEDK 2024Set 2024-M1 markMCQQ.If ∫sin3xcosx1dx=tanxk+c then the value of k is (A) −2 (B) 1 (C) 2 (D) −1
›Reveal solutionSolution
The integral simplifies by rewriting the integrand in terms of tanx, leading to a straightforward power rule integration; comparing the result with the given form shows k=−2.
We are given
∫sin3xcosx1dx=tanxk+c
and need to find k.
Concept and intuition
The integrand mixes powers of sinx and cosx. A classic trick is to express everything in terms of tanx (or cotx) because the derivative of tanx is sec2x, which itself is 1/cos2x. This often turns messy trigonometric integrals into simple power rules. Here, the presence of tanx on the right side is a strong hint: the integrand likely simplifies to something like (tanx)−3/2⋅sec2x, whose antiderivative is a constant times (tanx)−1/2.
Let’s work it out step by step.
- Rewrite the integrand using tanx.
sin3xcosx1=sin3/2x⋅cos1/2x1
Divide numerator and denominator by cos3/2x (a common trick to introduce tanx):
=cos3/2x⋅tan3/2x⋅cos1/2x1=cos2x⋅tan3/2x1
because cos3/2x⋅cos1/2x=cos2x.
Since 1/cos2x=sec2x, we have:
sin3xcosx1=tan3/2xsec2x.
- Set up the substitution. Let u=tanx. Then du=sec2xdx. The integral becomes:
∫tan3/2xsec2xdx=∫u3/2du=∫u−3/2du.
- Integrate using the power rule. ∫u−3/2du=−3/2+1u−3/2+1=−1/2u−1/2=−2u−1/2+C. …
- COMEDK 2021Set 20211 markMCQQ.∫1−4x2xdx is equal to (A) (log2)sin−12x+C (B) 21sin−12x+C (C) log21sin−12x+C (D) 2log2sin−12x+C
›Reveal solutionSolution
I = (1/log 2) * integral du / sqrt(1 - u^2) = (1/log 2) * arcsin(u) + C = (1/log 2) * arcsin(2^x) + C.
Concept: substitution reducing the integrand to the standard form 1/sqrt(1 - u^2), whose integral is arcsin(u).
I = integral 2^x / sqrt(1 - 4^x) dx. Note 4^x = (2^x)^2.
Put u = 2^x. Then du = 2^x * log 2 dx, so 2^x dx = du / log 2. …
- COMEDK 2021Set 20211 markMCQQ.Integral of ∫x2[1+x4]3/4dx. (A) −4(x1/4+1)1/4+C (B) 4(x1/4+1)1/4+C (C) 4(x4+1)1/4+C (D) None of these
›Reveal solutionSolution
The result -(x^4 + 1)^(1/4)/x + C matches none of options (A), (B), (C) (they are missing the 1/x factor, and (A)/(B) even have x^(1/4)).
Concept: for integrands of the form 1/(x^2 (1 + x^4)^(3/4)), take x^4 out of the bracket and substitute u = 1 + x^(-4).
(1 + x^4)^(3/4) = x^3 (1 + x^(-4))^(3/4) (for x > 0).
So the integrand = 1 / [ x^2 * x^3 * (1 + x^(-4))^(3/4) ] = x^(-5) (1 + x^(-4))^(-3/4).
Let u = 1 + x^(-4) => du = -4 x^(-5) dx => x^(-5) dx = -du/4.
I = -(1/4) * integral u^(-3/4) du = -(1/4) * (u^(1/4)/(1/4)) + C = -u^(1/4) + C
= -(1 + x^(-4))^(1/4) + C
= -((x^4 + 1)/x^4)^(1/4) + C
= -(x^4 + 1)^(1/4) / x + C.
Check by differentiating: d/dx [ -(1 + x^4)^(1/4) x^(-1) ] = -(1/4)(1 + x^4)^(-3/4)(4x^3)x^(-1) + (1 + x^4)^(1/4) x^(-2) …
- COMEDK 2023Set 2023-M1 markMCQQ.∫1−16x4xdx is equal to (A) (log4)sin−14x+C (B) 41sin−1(4x)+C (C) log41sin−14x+C (D) 4log4sin−14+C
›Reveal solutionSolution
Put u=4x so 16x=u2 and du=4xln4dx; the integral becomes ln41∫1−u2du=log41sin−1(4x)+C.
∫1−16x4xdx. Let u=4x⇒du=4xln4dx⇒4xdx=ln4du, and 16x=(4x)2=u2: …
- COMEDK 2025Set 2025-A1 markMCQQ.∫(1+x2)etan−1x(1+x+x2)dx= (A) etan−1x+c (B) xetan−1x+c (C) (1+x2)etan−1x+c (D) (1+x2)xetan−1x+c
›Reveal solutionSolution
The integral simplifies by substituting u=tan−1x, which turns the expression into a sum of a standard exponential integral and a derivative-of-product pattern, yielding xetan−1x+C. The correct option is (B).
The key insight is that the denominator 1+x2 is exactly the derivative of tan−1x, so the substitution u=tan−1x is natural. Once we do that, the polynomial 1+x+x2 becomes something in terms of tanu, and we can split the integral into two recognizable pieces.
- Substitute u=tan−1x. Then du=1+x2dx, and x=tanu. The integral becomes
∫etan−1x⋅1+x21+x+x2dx=∫eu(1+tanu+tan2u)du.
- Simplify the trigonometric expression. Recall 1+tan2u=sec2u. So
1+tanu+tan2u=sec2u+tanu.
The integral is now
∫eu(sec2u+tanu)du.
- Split and recognize patterns.
∫eusec2udu+∫eutanudu.
Notice that dud(tanu)=sec2u. The first integral is of the form ∫euf′(u)du with f(u)=tanu, and the second is ∫euf(u)du.
- Use the product rule in reverse. For any differentiable f(u),
dud(euf(u))=euf′(u)+euf(u).
Here f(u)=tanu, so
- COMEDK 2021Set 2021-B1 markMCQQ.If ∫1−4x2xdx=ksin−1(2x)+c, then k is (A) 2log2 (B) log21 (C) 2log21 (D) log2
›Reveal solutionSolution
k=log21.
Let u=2x, so du=2xln2dx and 4x=u2. Then
∫1−4x2xdx=∫1−u2u⋅uln2du=ln21∫1−u2du=ln21sin−1u+c. …
- COMEDK 2026Set 2026-M1 markMCQQ.
[!FORMULA] ∫x(1+xex)x+1dx=
(A) log∣cxex(1+xex)∣ (B) log∣cxex(1+xex)∣ (C) logxexc(1+xex) (D) log1+xexcxex›Reveal solutionSolution
The integral simplifies by noticing the derivative of xex appears in the denominator; the result is log1+xexcxex, which matches option (D).
The key insight is that the integrand contains xex in the denominator, and the derivative of xex is ex(1+x). That derivative is almost exactly the numerator x+1, except for a factor of ex. This suggests a substitution or a clever split of the fraction to reveal a logarithmic derivative.
- Rewrite the integrand to expose the derivative of xex. Notice that
dxd(xex)=ex+xex=ex(1+x).
Our numerator is x+1, so we can write:
x(1+xex)x+1=ex⋅x(1+xex)ex(x+1)=xex(1+xex)ex(1+x).
The numerator is now exactly the derivative of xex.
- Perform a substitution. Let t=xex. Then dt=ex(1+x)dx. The integral becomes:
∫xex(1+xex)ex(1+x)dx=∫t(1+t)dt.
- Decompose the rational function. Use partial fractions:
t(1+t)1=t1−1+t1.
So the integral is:
∫(t1−1+t1)dt=log∣t∣−log∣1+t∣+C=log1+tt+C.
- Substitute back. Since t=xex, we have: ∫x(1+xex)x+1dx=log1+xexxex+C. …
- COMEDK 2026Set 2026-M1 markMCQQ.
[!FORMULA] ∫x2+x21elog(1+x21)dx=
(A) 21tan−1(x2x2+1)+C (B) 21tan−1(2xx2−1)+C (C) −21tan−1(x−x1)+C (D) 21tan−1(x−x1)+C›Reveal solutionSolution
The integrand simplifies dramatically using exponent rules and algebraic manipulation, leading to a standard arctangent integral; the correct antiderivative matches option (D).
We start with the integral
∫x2+x21elog(1+x21)dx.
Concept & Intuition
The presence of elog(⋯) is a huge clue: for any positive argument, elog(u)=u. That immediately collapses the numerator into something algebraic. Then the denominator is symmetric in x and 1/x, which often suggests a substitution like t=x−1/x because its derivative appears in the numerator. This is a classic trick for integrals involving x2+1/x2.
Step-by-step solution
- Simplify the exponential Since elog(u)=u for u>0 (and 1+1/x2>0 for all real x=0), we have
elog(1+x21)=1+x21.
So the integral becomes
∫x2+x211+x21dx.
- Rewrite numerator and denominator Multiply numerator and denominator by x2 to clear fractions:
x2+x211+x21=x4+1x2+1.
So the integral is
∫x4+1x2+1dx.
- Divide numerator and denominator by x2 This is the key algebraic trick:
x4+1x2+1=x2+x211+x21.
Notice that the numerator 1+1/x2 is the derivative of x−1/x (since dxd(x−1/x)=1+1/x2).
Also, x2+1/x2=(x−1/x)2+2.
- Substitute Let t=x−x1. Then
dt=(1+x21)dx.
And
x2+x21=t2+2.
The integral becomes
∫t2+2dt.
- Integrate This is a standard arctangent form:
∫t2+a2dt=a1tan−1(at)+C.
Here a=2, so
∫t2+2dt=21tan−1(2t)+C.
- Back-substitute Replace t with x−x1:
21tan−1(2x−x1)+C.
Simplify the argument:
2x−x1=2xx2−1.
So the antiderivative is
21tan−1(2xx2−1)+C. …
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