Applications of IntegrationTopic #27 of 32

Improper Integrals

Evaluating integrals with infinite limits or discontinuities.

Types of Improper Integrals

Type 1: Infinite Limits

∫a∞f(x) dx=lim⁡t→∞∫atf(x) dx\int_a^\infty f(x) \, dx = \lim_{t \to \infty} \int_a^t f(x) \, dx

∫−∞bf(x) dx=lim⁡t→−∞∫tbf(x) dx\int_{-\infty}^b f(x) \, dx = \lim_{t \to -\infty} \int_t^b f(x) \, dx

∫−∞∞f(x) dx=∫−∞cf(x) dx+∫c∞f(x) dx\int_{-\infty}^\infty f(x) \, dx = \int_{-\infty}^c f(x) \, dx + \int_c^\infty f(x) \, dx

Type 2: Discontinuous Integrands

If ff has a discontinuity at cc in [a,b][a, b]:

∫abf(x) dx=lim⁡t→c−∫atf(x) dx+lim⁡s→c+∫sbf(x) dx\int_a^b f(x) \, dx = \lim_{t \to c^-} \int_a^t f(x) \, dx + \lim_{s \to c^+} \int_s^b f(x) \, dx

If ff is discontinuous at aa:

∫abf(x) dx=lim⁡t→a+∫tbf(x) dx\int_a^b f(x) \, dx = \lim_{t \to a^+} \int_t^b f(x) \, dx

If ff is discontinuous at bb:

∫abf(x) dx=lim⁡t→b−∫atf(x) dx\int_a^b f(x) \, dx = \lim_{t \to b^-} \int_a^t f(x) \, dx

Convergence and Divergence

  • Converges: if the limit exists and is finite
  • Diverges: if the limit is ±∞\pm\infty or doesn't exist

Important Result: p-Integral

∫1∞1xp dx={1p−1if p>1 (converges)divergesif p≤1\int_1^\infty \frac{1}{x^p} \, dx = \begin{cases} \frac{1}{p-1} & \text{if } p > 1 \text{ (converges)} \\ \text{diverges} & \text{if } p \leq 1 \end{cases}

∫011xp dx={11−pif p<1 (converges)divergesif p≥1\int_0^1 \frac{1}{x^p} \, dx = \begin{cases} \frac{1}{1-p} & \text{if } p < 1 \text{ (converges)} \\ \text{diverges} & \text{if } p \geq 1 \end{cases}

Comparison Test

If 0≤f(x)≤g(x)0 \leq f(x) \leq g(x) for x≥ax \geq a:

  • If ∫a∞g(x) dx\int_a^\infty g(x) \, dx converges, then ∫a∞f(x) dx\int_a^\infty f(x) \, dx converges
  • If ∫a∞f(x) dx\int_a^\infty f(x) \, dx diverges, then ∫a∞g(x) dx\int_a^\infty g(x) \, dx diverges

Examples

Example 1: Infinite upper limit

∫1∞1x2 dx=lim⁡t→∞∫1tx−2 dx\int_1^\infty \frac{1}{x^2} \, dx = \lim_{t \to \infty} \int_1^t x^{-2} \, dx

=lim⁡t→∞[−1x]1t= \lim_{t \to \infty} \left[-\frac{1}{x}\right]_1^t

=lim⁡t→∞(−1t+1)= \lim_{t \to \infty} \left(-\frac{1}{t} + 1\right)

=0+1=1= 0 + 1 = 1

Converges to 1.

Example 2: Infinite lower limit

∫−∞0ex dx=lim⁡t→−∞∫t0ex dx\int_{-\infty}^0 e^x \, dx = \lim_{t \to -\infty} \int_t^0 e^x \, dx

=lim⁡t→−∞[ex]t0= \lim_{t \to -\infty} \left[e^x\right]_t^0

=lim⁡t→−∞(1−et)= \lim_{t \to -\infty} (1 - e^t)

=1−0=1= 1 - 0 = 1

Converges to 1.

Example 3: Both limits infinite

∫−∞∞11+x2 dx\int_{-\infty}^\infty \frac{1}{1+x^2} \, dx

=∫−∞011+x2 dx+∫0∞11+x2 dx= \int_{-\infty}^0 \frac{1}{1+x^2} \, dx + \int_0^\infty \frac{1}{1+x^2} \, dx

=lim⁡t→−∞[arctan⁡(x)]t0+lim⁡s→∞[arctan⁡(x)]0s= \lim_{t \to -\infty} \left[\arctan(x)\right]_t^0 + \lim_{s \to \infty} \left[\arctan(x)\right]_0^s

=(0−(−π2))+(π2−0)= \left(0 - \left(-\frac{\pi}{2}\right)\right) + \left(\frac{\pi}{2} - 0\right)

=π= \pi

Example 4: Discontinuity at endpoint

∫011x dx=lim⁡t→0+∫t1x−1/2 dx\int_0^1 \frac{1}{\sqrt{x}} \, dx = \lim_{t \to 0^+} \int_t^1 x^{-1/2} \, dx

=lim⁡t→0+[2x]t1= \lim_{t \to 0^+} \left[2\sqrt{x}\right]_t^1

=lim⁡t→0+(2−2t)= \lim_{t \to 0^+} (2 - 2\sqrt{t})

=2−0=2= 2 - 0 = 2

Example 5: Discontinuity in interior

∫031(x−1)2/3 dx\int_0^3 \frac{1}{(x-1)^{2/3}} \, dx

Split at x=1x = 1:

=∫011(x−1)2/3 dx+∫131(x−1)2/3 dx= \int_0^1 \frac{1}{(x-1)^{2/3}} \, dx + \int_1^3 \frac{1}{(x-1)^{2/3}} \, dx

First: lim⁡t→1−[3(x−1)1/3]0t=lim⁡t→1−(3(t−1)1/3+3)=3\lim_{t \to 1^-} \left[3(x-1)^{1/3}\right]_0^t = \lim_{t \to 1^-} (3(t-1)^{1/3} + 3) = 3

Second: lim⁡s→1+[3(x−1)1/3]s3=3(2)1/3−0=323\lim_{s \to 1^+} \left[3(x-1)^{1/3}\right]_s^3 = 3(2)^{1/3} - 0 = 3\sqrt[3]{2}

Total: 3+3233 + 3\sqrt[3]{2}

Example 6: Divergent integral

∫1∞1x dx=lim⁡t→∞[ln⁡∣x∣]1t\int_1^\infty \frac{1}{x} \, dx = \lim_{t \to \infty} \left[\ln|x|\right]_1^t

=lim⁡t→∞(ln⁡(t)−0)= \lim_{t \to \infty} (\ln(t) - 0)

=∞= \infty

Diverges.

Example 7: Using comparison

∫1∞e−x2 dx\int_1^\infty e^{-x^2} \, dx

Since e−x2<e−xe^{-x^2} < e^{-x} for x>1x > 1:

∫1∞e−x dx=lim⁡t→∞[−e−x]1t=0+e−1=1e (converges)\int_1^\infty e^{-x} \, dx = \lim_{t \to \infty} \left[-e^{-x}\right]_1^t = 0 + e^{-1} = \frac{1}{e} \text{ (converges)}

Therefore ∫1∞e−x2 dx\int_1^\infty e^{-x^2} \, dx also converges.