Improper Integrals with Infinite Discontinuities

An improper integral with an infinite discontinuity has an integrand that blows up at an endpoint or inside the interval, like \int_0^1 \dfrac{1}{\sqrt{x}}\,dx. Replace the bad point with t, integrate, and take a one-sided limit. A finite limit means the integral converges; otherwise it diverges.

Before this lesson: Improper Integrals, One-Sided Limits and Infinite Limits

Area next to a vertical asymptote

The graph of y = 1/√x shoots up as x gets close to 0. The region under it from 0 to 1 is infinitely tall, yet its area is exactly 2. The region is tall but very thin near the asymptote.

The danger is that these integrals look normal. \int_{-1}^{1} \dfrac{1}{x^2}\,dx has ordinary-looking limits, but 1/x² blows up at x = 0. Always check where the integrand is undefined before you integrate.

Graph of y = 1/√x for x from 0 to 4. The curve rises without bound as x approaches 0, next to the y-axis, which is a vertical asymptote. The region under the curve from x = 0 to x = 1 is shaded and labeled area = 2.
The shaded region is infinitely tall near x = 0, but its area is finite: 2.

Definitions for infinite discontinuities

If f is continuous on [a, b) and blows up at b, or continuous on (a, b] and blows up at a:

\int_a^b f(x)\,dx = \lim_{t \to b^-} \int_a^t f(x)\,dx \qquad \int_a^b f(x)\,dx = \lim_{t \to a^+} \int_t^b f(x)\,dx

If f blows up at a point c inside [a, b], split the integral at c. It converges only if both pieces converge.

\int_a^b f(x)\,dx = \int_a^c f(x)\,dx + \int_c^b f(x)\,dx

The p-rule near 0: \int_0^1 \dfrac{1}{x^p}\,dx converges to \dfrac{1}{1 - p} if p is less than 1 and diverges if p ≥ 1. This is the reverse of the rule for \int_1^{\infty}.

Improper integral examples with infinite discontinuities

Example 1: Blowing up at the left end

Evaluate \int_0^1 \dfrac{1}{\sqrt{x}}\,dx.

\int_0^1 x^{-1/2}\,dx = \lim_{t \to 0^+} \int_t^1 x^{-1/2}\,dx

The integrand blows up at 0, so replace 0 with t.

= \lim_{t \to 0^+} \Big[2\sqrt{x}\Big]_t^1

Integrate with the power rule (see antiderivatives).

= \lim_{t \to 0^+} (2 - 2\sqrt{t})

Plug in 1 and t.

= 2 - 0 = 2

√t → 0.

Answer: the integral converges to 2.

Example 2: A divergent one

Evaluate \int_0^1 \dfrac{1}{x^2}\,dx.

\int_0^1 x^{-2}\,dx = \lim_{t \to 0^+} \Big[-\dfrac{1}{x}\Big]_t^1

Replace 0 with t and integrate.

= \lim_{t \to 0^+} \left(-1 + \dfrac{1}{t}\right)

Plug in 1 and t.

= \infty

1/t grows without bound as t → 0⁺.

Answer: the integral diverges. Here p = 2 ≥ 1.

Example 3: A discontinuity inside the interval

Evaluate \int_0^3 \dfrac{1}{(x - 1)^{2/3}}\,dx.

(x - 1)^{2/3} = 0 \text{ at } x = 1

The integrand blows up at x = 1, inside [0, 3].

\int (x - 1)^{-2/3}\,dx = 3(x - 1)^{1/3} + C

Power rule with u = x − 1.

\int_0^1 = \lim_{t \to 1^-} \Big[3(x - 1)^{1/3}\Big]_0^t = 0 - 3(-1) = 3

Left piece; the cube root of −1 is −1 (see cube roots).

\int_1^3 = \lim_{t \to 1^+} \Big[3(x - 1)^{1/3}\Big]_t^3 = 3\sqrt[3]{2} - 0

Right piece.

3 + 3\sqrt[3]{2} \approx 6.780

Both pieces converge, so add them.

Answer: the integral converges to 3 + 3\sqrt[3]{2} \approx 6.780.

Example 4: A logarithm at 0

Evaluate \int_0^1 \ln x\,dx.

\int \ln x\,dx = x\ln x - x + C

Use parts with u = ln x and dv = dx (see integration by parts).

\int_0^1 \ln x\,dx = \lim_{t \to 0^+} \Big[x\ln x - x\Big]_t^1

ln x blows up at 0, so use a limit.

= \lim_{t \to 0^+} \big[(0 - 1) - (t\ln t - t)\big]

Plug in 1 and t; ln 1 = 0.

\lim_{t \to 0^+} t\ln t = \lim_{t \to 0^+} \dfrac{\ln t}{1/t} = \lim_{t \to 0^+} \dfrac{1/t}{-1/t^2} = \lim_{t \to 0^+} (-t) = 0

Rewrite as ∞/∞ and use L’Hôpital’s rule (see L’Hôpital’s rule).

= -1 - (0 - 0) = -1

Finish the limit.

Answer: the integral converges to −1. It is negative because ln x is negative on (0, 1).

Example 5: A tank that drains faster and faster

Water drains from a tank at a rate of r(t) = \dfrac{6}{\sqrt{4 - t}} liters per minute for t from 0 up to 4. The rate blows up as t nears 4 minutes. How much water drains in those 4 minutes?

\int_0^4 6(4 - t)^{-1/2}\,dt = \lim_{b \to 4^-} \int_0^b 6(4 - t)^{-1/2}\,dt

The rate blows up at t = 4.

\int 6(4 - t)^{-1/2}\,dt = -12\sqrt{4 - t} + C

Let u = 4 − t, so du = −dt (see u-substitution).

= \lim_{b \to 4^-} \left(-12\sqrt{4 - b} + 12\sqrt{4}\right)

Plug in b and 0.

= 0 + 24 = 24

√(4 − b) → 0, and 12 · 2 = 24.

Answer: 24 liters drain, even though the rate becomes infinite.

Common mistakes

MistakeExample of the errorFix
Missing a discontinuity inside\int_{-1}^{1} \dfrac{1}{x^2}\,dx = \Big[-\dfrac{1}{x}\Big]_{-1}^{1} = -21/x² blows up at 0. Split there; \int_0^1 \dfrac{1}{x^2}\,dx diverges, so the whole integral diverges.
Using the wrong p-rule\int_0^1 \dfrac{1}{x^2}\,dx converges since p = 2 is more than 1Near 0 the rule flips: it converges only when p is less than 1.
Letting the pieces cancel\int_{-1}^{1} \dfrac{1}{x}\,dx = 0 by symmetryEach piece diverges on its own, so the integral diverges.
Wrong side of the limit\lim_{t \to 0^-} for \int_0^1The interval is to the right of 0, so use t → 0⁺.
Plugging in the bad point\Big[x\ln x - x\Big]_0^1 with ln 0ln 0 is undefined. Use a limit as t → 0⁺.

Related methods

Both kinds at once

Some integrals are improper in two ways, like \int_0^{\infty} \dfrac{1}{\sqrt{x}(1 + x)}\,dx. Split it at a point such as x = 1, so each piece has only one problem, and check each piece. This one converges to π.

Deciding without an antiderivative

If you can’t integrate, compare. Near the bad point, an integrand smaller than a convergent p-integral also converges. That is the comparison test, the next lesson.

The p-rule near 0

For p ≠ 1, \int_t^1 x^{-p}\,dx = \dfrac{1 - t^{1-p}}{1 - p}. If p is less than 1, t¹⁻ᵖ → 0 and the integral approaches 1/(1 − p). If p is more than 1, t¹⁻ᵖ → ∞. For p = 1, you get −ln t → ∞.

Practice problems

Decide whether each integral converges or diverges. If it converges, find its value.

  1. \int_0^4 \dfrac{1}{\sqrt{x}}\,dx
  2. \int_0^1 \dfrac{1}{x}\,dx
  3. \int_0^8 x^{-1/3}\,dx
  4. \int_1^2 \dfrac{1}{x - 1}\,dx
  5. \int_0^2 \dfrac{1}{\sqrt{2 - x}}\,dx
  6. \int_{-1}^{1} \dfrac{1}{x^{2/3}}\,dx
  7. \int_0^{\pi/2} \tan x\,dx
  8. \int_0^1 x\ln x\,dx
  9. \int_0^1 \dfrac{1}{\sqrt{1 - x^2}}\,dx
  10. Use the p-rule to find \int_0^1 x^{-0.9}\,dx.
Show answers

1.

\lim_{t \to 0^+} \Big[2\sqrt{x}\Big]_t^4

Replace 0 with t and integrate.

= \lim_{t \to 0^+} (4 - 2\sqrt{t}) = 4

Plug in; √t → 0.

Answer: converges to 4

2.

\lim_{t \to 0^+} \Big[\ln x\Big]_t^1 = \lim_{t \to 0^+} (0 - \ln t)

Integrate 1/x and plug in.

= \infty

ln t → −∞ as t → 0⁺.

Answer: diverges

3.

\lim_{t \to 0^+} \Big[\tfrac{3}{2}x^{2/3}\Big]_t^8

Integrate x^(−1/3).

= \tfrac{3}{2}(8)^{2/3} - 0 = \tfrac{3}{2}(4) = 6

8^(2/3) = 4 (see rational exponents).

Answer: converges to 6

4.

\lim_{t \to 1^+} \Big[\ln(x - 1)\Big]_t^2 = \lim_{t \to 1^+} \big(0 - \ln(t - 1)\big)

Integrate and plug in; ln 1 = 0.

= \infty

ln(t − 1) → −∞.

Answer: diverges

5.

\lim_{t \to 2^-} \Big[-2\sqrt{2 - x}\Big]_0^t

Integrate with u = 2 − x.

= \lim_{t \to 2^-} \left(-2\sqrt{2 - t} + 2\sqrt{2}\right) = 2\sqrt{2}

√(2 − t) → 0.

Answer: converges to 2√2 ≈ 2.828

6.

\int x^{-2/3}\,dx = 3x^{1/3} + C

Blows up at 0, inside [−1, 1].

\int_{-1}^{0} = 0 - 3(-1) = 3, \quad \int_0^1 = 3 - 0 = 3

Each piece is a limit at 0.

3 + 3 = 6

Both converge, so add.

Answer: converges to 6

7.

\int \tan x\,dx = -\ln(\cos x) + C

On (0, π/2), cos x is positive (see integrals that give natural logarithms).

\lim_{t \to \pi/2^-} \big(-\ln(\cos t) + \ln 1\big) = \infty

cos t → 0⁺, so ln(cos t) → −∞.

Answer: diverges

8.

\int x\ln x\,dx = \dfrac{x^2}{2}\ln x - \dfrac{x^2}{4} + C

Parts with u = ln x, dv = x dx.

\lim_{t \to 0^+} \left[\left(0 - \dfrac{1}{4}\right) - \left(\dfrac{t^2}{2}\ln t - \dfrac{t^2}{4}\right)\right]

Plug in 1 and t.

= -\dfrac{1}{4} - 0 = -\dfrac{1}{4}

t² ln t → 0 by L’Hôpital’s rule.

Answer: converges to −1/4

9.

\lim_{t \to 1^-} \Big[\arcsin x\Big]_0^t = \lim_{t \to 1^-} \arcsin t - 0

The integrand blows up at 1 (see integrals that give inverse trig functions).

= \dfrac{\pi}{2}

arcsin 1 = π/2.

Answer: converges to π/2

10.

p = 0.9, \text{ which is less than } 1

The p-rule near 0 applies.

\dfrac{1}{1 - 0.9} = \dfrac{1}{0.1} = 10

Use 1/(1 − p).

Answer: converges to 10

Infinite discontinuities FAQ

What is an infinite discontinuity in an integral?

It is a point where the integrand blows up to ±∞, usually at a vertical asymptote. If it lies in the interval, the integral is improper.

How do you evaluate an improper integral with a vertical asymptote?

Replace the bad point with t, integrate, and take a one-sided limit toward it. If the asymptote is inside the interval, split there and do each side.

Does the integral of 1/x from 0 to 1 converge?

No. It equals the limit of −ln t as t → 0⁺, which is infinite, so it diverges.

Can you integrate 1/x² from −1 to 1?

Not as a normal integral, because 1/x² blows up at 0. Split at 0. Each piece diverges, so the integral diverges. The answer −2 from plugging in is wrong.

Summary

  • Check where the integrand blows up before integrating.
  • Replace the bad point with t and take a one-sided limit.
  • Split at a bad point inside the interval; both pieces must converge.
  • ∫ from 0 to 1 of 1/xᵖ converges only when p is less than 1, to 1/(1 − p).
  • An infinitely tall region can still have a finite area.

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