Practice: Techniques of Integration

Recognition · Error diagnosis

A learner writes: " ∫ 1 ∞ d x x = [ ln ⁡ x ] 1 ∞ = ln ⁡ ∞ − ln ⁡ 1 , and since ln ⁡ 1 = 0 the answer is ln ⁡ ∞ ."

What is wrong?

2 hints available, least help first.

Hint 1: Retrieval cue

What does the notation ∫ 1 ∞ abbreviate?

Hint 2: Concept cue

Replace the upper limit by t , evaluate, then ask what happens as t → ∞ .

Direct application

Evaluate ∫ 1 e ln ⁡ x d x using integration by parts.

Enter the value. It is checked against the answer and the precision this task asks for.

2 hints available, least help first.

Hint 1: Retrieval cue

There is only one factor, so what should d v be?

Hint 2: Concept cue

With d v = d x and u = ln ⁡ x , the antiderivative is x ln ⁡ x − x .

Direct application

Decompose 1 ( x − 1 ) ( x + 2 ) as A x − 1 + B x + 2 .

Give the value of A as a decimal.

Enter the value. It is checked against the answer and the precision this task asks for.

2 hints available, least help first.

Hint 1: Retrieval cue

Multiply both sides by ( x − 1 ) ( x + 2 ) , then choose an x that removes one unknown.

Hint 2: Concept cue

Substituting x = 1 leaves 1 = 3 A .

Direct application

Evaluate ∫ 0 ∞ e − x d x by writing it as a limit.

Enter the value. It is checked against the answer and the precision this task asks for.

2 hints available, least help first.

Hint 1: Retrieval cue

Replace the infinite limit by t and evaluate the resulting proper integral.

Hint 2: Concept cue

The antiderivative is − e − x , giving 1 − e − t . What happens to e − t ?

Classification · Direct application

Consider these four integrals:

∫ 1 ∞ d x x 1 / 2 , ∫ 1 ∞ d x x , ∫ 1 ∞ d x x 3 / 2 , ∫ 1 ∞ d x x 3

How many of them converge?

Enter the value. It is checked against the answer and the precision this task asks for.

2 hints available, least help first.

Hint 1: Retrieval cue

What is the threshold value of p for convergence at infinity, and which side of it converges?

Hint 2: Concept cue

Convergence needs p > 1 . Check each exponent against that, remembering p = 1 itself diverges.

Method selection · Classification

Which technique does ∫ 2 x x 2 + 1 d x call for?

2 hints available, least help first.

Hint 1: Retrieval cue

Differentiate the denominator. Does the result appear in the numerator?

Hint 2: Concept cue

d d x ( x 2 + 1 ) = 2 x , which is exactly the numerator.

Construction · Direct application · Explanation

(a) Evaluate ∫ 1 2 x ln ⁡ x d x , stating which factor you take as u and why.

(b) Evaluate ∫ 3 5 d x ( x − 1 ) ( x + 2 ) by partial fractions, verifying the decomposition at one value of x .

(c) Decide whether ∫ 0 1 d x x converges, and evaluate it if it does.

(d) Decide whether ∫ 1 ∞ d x x 3 converges, and evaluate it if it does. State the general threshold your reasoning uses.

(e) A learner evaluates ∫ − 1 1 d x x 2 as [ − 1 x ] − 1 1 = − 1 − 1 = − 2 . Give two independent reasons the answer cannot be right, say which hypothesis was violated, and carry out the evaluation correctly.

Write your answer, then compare it with the worked solution.

3 hints available, least help first.

Hint 1: Retrieval cue

Before evaluating anything, check each integral for an infinite limit or an unbounded integrand.

Hint 2: Concept cue

In (a), choose as u the factor that gets simpler when differentiated.

Hint 3: Strategy cue

In (e), compare the sign of the integrand with the sign of the reported answer.

Compare with the worked solution

Comparing does not record a result. Judging your own written answer cannot show that you can do this without help.

(a) ∫ 1 2 x ln ⁡ x d x by parts. Take u = ln ⁡ x and d v = x d x . The reason is that ln ⁡ x simplifies when differentiated, becoming 1 / x , while x is trivial to integrate. The reverse choice would leave a logarithm to integrate and a higher power of x , which is worse. So d u = d x x and v = x 2 2 :

∫ 1 2 x ln ⁡ x d x = [ x 2 2 ln ⁡ x ] 1 2 − ∫ 1 2 x 2 2 ⋅ 1 x d x = ( 2 ln ⁡ 2 − 0 ) − ∫ 1 2 x 2 d x .

The 1 / x cancelled against x 2 , which is the whole point of the choice. Finishing:

∫ 1 2 x 2 d x = [ x 2 4 ] 1 2 = 1 − 1 4 = 3 4 ,
∫ 1 2 x ln ⁡ x d x = 2 ln ⁡ 2 − 3 4 ≈ 0.6362943611 .

Check: differentiating x 2 2 ln ⁡ x − x 2 4 gives x ln ⁡ x + x 2 − x 2 = x ln ⁡ x ✓. A midpoint sum returns 0.6362943611 ✓. (b) ∫ 3 5 d x ( x − 1 ) ( x + 2 ) by partial fractions. The integrand is proper, numerator degree 0, denominator degree 2, so decompose directly:

1 ( x − 1 ) ( x + 2 ) = A x − 1 + B x + 2 ⟹ 1 = A ( x + 2 ) + B ( x − 1 ) .

Substituting the roots isolates each coefficient: at x = 1 , 1 = 3 A so A = 1 3 ; at x = − 2 , 1 = − 3 B so B = − 1 3 . Verification at x = 3 : the original is 1 2 ⋅ 5 = 0.1 ; the decomposition gives 1 / 3 2 − 1 / 3 5 = 1 6 − 1 15 = 0.1 ✓. Integrating term by term:

1 3 [ ln ⁡ | x − 1 | − ln ⁡ | x + 2 | ] 3 5 = 1 3 [ ln ⁡ x − 1 x + 2 ] 3 5 = 1 3 ( ln ⁡ 4 7 − ln ⁡ 2 5 ) = 1 3 ln ⁡ 10 7 ≈ 0.1188916480 .

Check: a midpoint sum returns 0.1188916480 ✓. (c) ∫ 0 1 d x x — improper at the left endpoint. The integrand is unbounded as x → 0 + , so the integral is improper and is defined as a limit:

∫ 0 1 x − 1 / 2 d x = lim s → 0 + ∫ s 1 x − 1 / 2 d x = lim s → 0 + [ 2 x ] s 1 = lim s → 0 + ( 2 − 2 s ) = 2 .

It converges, to 2. Check: the partial values are 1.3675 at s = 0.1 , 1.9368 at s = 0.001 , 1.9980 at s = 10 − 6 ✓. By the p-test near zero: ∫ 0 1 x − p d x converges when p < 1 , and here p = 1 2 ✓. the region is unbounded in height and has finite area. Unboundedness alone never decides convergence. (d) ∫ 1 ∞ d x x 3 — improper at infinity.

∫ 1 ∞ x − 3 d x = lim t → ∞ [ − 1 2 x 2 ] 1 t = lim t → ∞ ( 1 2 − 1 2 t 2 ) = 1 2 .

It converges, to 1 2 . The threshold. ∫ 1 ∞ x − p d x converges exactly when p > 1 , with value 1 p − 1 ; here p = 3 gives 1 2 ✓. The case p = 1 diverges, since the antiderivative ln ⁡ t grows without bound. The two thresholds run opposite ways, p > 1 at infinity, p < 1 at zero, because at infinity the integrand must decay fast enough, while near zero it must blow up slowly enough. p = 1 fails at both ends. (e) The invalid evaluation of ∫ − 1 1 x − 2 d x . Two independent reasons the answer cannot be right. 1. The sign is impossible. 1 / x 2 > 0 everywhere it is defined, so every Riemann term is positive and any value must be positive. The reported − 2 contradicts the construction before any theorem is consulted.
2. The integral diverges. Near 0 the integrand is unbounded, and the accumulated area grows without limit, so no finite number can be the answer. The hypothesis violated. Part 2 of the fundamental theorem requires F to be an antiderivative of f on the whole closed interval. Neither f ( x ) = x − 2 nor F ( x ) = − 1 / x is defined at x = 0 ∈ [ − 1 , 1 ] , so F is not an antiderivative there and the theorem does not apply. The arithmetic proceeded regardless, which is what produced a number. The correct evaluation. The integrand is unbounded at an interior point, so split there and treat each piece as a limit:

∫ − 1 1 d x x 2 = ∫ − 1 0 d x x 2 + ∫ 0 1 d x x 2 .

For the right piece,

∫ 0 1 x − 2 d x = lim s → 0 + [ − 1 x ] s 1 = lim s → 0 + ( − 1 + 1 s ) = + ∞ ,

since 1 s − 1 reads 9 at s = 0.1 , 99 at s = 0.01 and 9999 at s = 10 − 4 . That piece diverges, and by symmetry so does the left one. Since one piece diverges, the whole integral diverges. The divergences do not cancel: convergence requires each piece to converge on its own. Pairing the two symmetrically to obtain 0 computes the Cauchy principal value, which is a different quantity and is not the integral. By the p-test: near zero, ∫ 0 1 x − p d x needs p < 1 , and here p = 2 ✓ diverges. The same conclusion without computing anything.

A complete answer does each of these:

  • applies integration by parts
  • decomposes partial fractions
  • evaluates improper as limit
  • applies p test
  • selects technique
  • explains convergence
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