Concept understanding — Improper Integral Evaluation
Improper Integral Evaluation
The Intuition First
You already know how to integrate over a finite interval: ∫13f(x)dx is the area under the curve from x=1 to x=3. But what if the region stretches to infinity, or the function shoots up to infinity somewhere in the interval?
That is what improper integrals handle — two situations that break the ordinary rules:
Infinite limits — integrating up to ∞ or down to −∞.
Infinite discontinuities — the function blows up at some point of the interval.
The core idea is the same in both cases: replace the "bad" point with a limit. Integrate up to a finite value, then let that value approach the trouble spot. If the result approaches a finite number, the integral converges; if it grows without bound, it diverges.
The Precise Definitions
Type 1: Infinite limits
∫a∞f(x)dx=limb→∞∫abf(x)dx
∫−∞bf(x)dx=lima→−∞∫abf(x)dx
For a doubly-infinite integral, split at a convenient point c and require both pieces to converge:
∫−∞∞f(x)dx=∫−∞cf(x)dx+∫c∞f(x)dx
Type 2: Infinite discontinuities
If f has a vertical asymptote at an endpoint, approach it from inside the interval:
If f blows up at x=a: ∫abf(x)dx=t→a+lim∫tbf(x)dx
If f blows up at x=b: ∫abf(x)dx=t→b−lim∫atf(x)dx
If the blow-up is at an interior point c, split at c and treat each side separately.
Never treat an improper integral as an ordinary one. Blindly applying the Fundamental Theorem across a discontinuity gives wrong answers. Always first check: is the integrand defined and finite on the whole interval? …
These are four ordinary definite integrals: power rule for (i), substitution for (ii) and (iv), partial fractions for (iii). The values are 319, 9919, log2732, and 81.
Each part is a proper definite integral (the integrand is finite on the whole interval), so we find an antiderivative and apply F(b)−F(a). The only skill is spotting the right technique for each.
(i) ∫23x2dx
Straight power rule: ∫xndx=n+1xn+1 with n=2.
∫23x2dx=[3x3]23=333−323=327−8=319.
(ii) ∫49(30−x3/2)2xdx
The derivative of the inner expression 30−x3/2 is −23x — a constant multiple of the numerator, which flags a substitution.
Method: Identify-the-Technique for Each Definite Integral, Then Apply Limits
Use this for a set of definite integrals of different types: choose the antiderivative technique per integrand, then evaluate with the Fundamental Theorem, ∫abf=F(b)−F(a).
Steps
Step 1: Classify each integrand.
Match to a technique: a plain power → power rule; a composite with its derivative present → substitution; a proper rational function → partial fractions.
Step 2: For a substitution, change the limits too. …
Mistake 1: Keeping the old x-limits after substituting.
Why it's wrong: once you change to u, the limits must become u-values; using the x-limits gives a wrong number. Correct approach: convert limits with u=g(a), u=g(b).
The substitution x=1/t maps this improper integral to its own negative, so by symmetry I=−I⇒I=0.
Concept and Intuition
When an integral over (0,∞) has an integrand that is "anti-symmetric" under the reciprocal map x→1/x (i.e., transforms into its own negative), the integral must vanish — this is a classic trick avoiding the need to actually evaluate divergent-looking pieces.
Step-by-Step Solution
Let h(x)=(x12+x−12)xlogx and I=∫0∞h(x)dx.
Substitute x=t1, so dx=−t21dt; as x:0→∞, t:∞→0.
x12+x−12=t−12+t12 (symmetric, unchanged in form). logx=−logt. xdx=1/t−dt/t2=−tdt.
So h(x)dx=(t12+t−12)(−logt)(−tdt)=(t12+t−12)tlogtdt... but we must also flip the limits of integration back from (∞,0) to (0,∞), which introduces one more overall minus sign.
Carrying the limit-flip sign through carefully: I=−∫0∞(t12+t−12)tlogtdt=−I.
Q.If M=∫0∞1+t3logtdt and N=∫−∞∞1+e3te2ttdt, then
(A) N=2M
(B) N=M
(C) N=3M
(D) N=−M
›Reveal solutionSolution
A substitution t=eu turns N into ∫0∞1+s3slogsds, and a substitution t→1/t in M shows this equals −M; so N=−M, option (D).
Concept and Intuition
N's integrand 1+e3te2tt is exactly what you get from 1+s3slogs under s=et — recognizing this lets us relate N back to an integral of the same shape as M, and then a reciprocal substitution inside M finishes the comparison.
Step-by-Step Solution
In N=∫−∞∞1+e3te2ttdt, substitute s=et (so t=logs, dt=ds/s, and as t:−∞→∞, s:0→∞):
N=∫0∞1+s3s2logs⋅sds=∫0∞1+s3slogsds.
Call this integral P=∫0∞1+s3slogsds, so N=P.
Now relate P to M=∫0∞1+t3logtdt by substituting s=1/u in P (ds=−du/u2; as s:0→∞, u:∞→0): …
Recognizing the integrand as the derivative of sinx/(cosx+xsinx) gives f explicitly, and its limit at π/2 is 2/π.
Concept and Intuition
Integrands of the form (xtanx+1)21 often come from quotient-rule differentiation of cosx+xsinxsinx — spotting this pattern avoids a messy substitution.
Step-by-Step Solution
Rewrite 1+xtanx=cosxcosx+xsinx, so the integrand is (cosx+xsinx)2cos2x.
Let D(x)=cosx+xsinx. Then D′(x)=−sinx+sinx+xcosx=xcosx.
A sum that looks unwieldy converts to a standard Riemann-sum limit; recognizing the 1/t integral gives the answer 2.
Concept and Intuition
Whenever you see n1∑f(k/n) (or an algebraically disguised version of it) as n→∞, it is begging to be converted into a definite integral ∫01f(t)dt. The trick here is to first pull the n inside the sum so every term becomes a function of k/n times 1/n.
Step-by-Step Solution
Write the expression as Sn=n1∑k=1nk1.
Multiply and divide inside: n1⋅k1=n1⋅kn=n1⋅k/n1.
So Sn=k=1∑nn1⋅k/n1, which is exactly the Riemann sum (right-endpoint) for f(t)=1/t on [0,1] with tk=k/n. …
This is a Riemann-sum-style limit: ∑kp/np+1→1/(p+1) as n→∞.
Concept and Intuition
The sum 1p+2p+⋯+np grows like ∫0nxpdx=p+1np+1 for large n — this can be seen directly by writing the ratio as a Riemann sum: n1∑k=1n(nk)p→∫01xpdx=p+11.