Properties of the Definite Integral

Flip the limits, and the sign flips too.

Reversing the limits

The integral from a to b of f(x) dx is F(b) − F(a). Run it the other way, from b to a, and it becomes F(a) − F(b), which is −(F(b) − F(a)). So swapping the limits changes the sign.

In strips: going from b back to a, each step is Δx = (a − b) / n, a negative width, so every term f(xᵢ) Δx changes sign and so does the sum.

Check it on y = x²/4, whose antiderivative is x³/12. From 0 to 2 the integral is 8/12 − 0 = 2/3. From 2 to 0 it is 0 − 8/12 = −2/3.

Equal limits

The integral from a to a is F(a) − F(a) = 0. There is no width, so there are no strips to add, whatever f is. The integral of any function from 3 to 3 is 0.

A constant factor comes out

Multiply every height by a constant k and every strip f(xᵢ) Δx becomes k f(xᵢ) Δx, so the whole sum is k times as big: ∫ k f(x) dx = k ∫ f(x) dx.

Check it: from 0 to 2, x²/4 has integral 2/3. Twice the function, x²/2, has antiderivative x³/6 and integral 8/6 = 4/3, which is 2 × 2/3. In the same way the integral of 3x² from 0 to 2 is 2³ = 8, and 3 times the integral of x², 3 × 8/3, is 8 as well.

xy

The gold curve y = x²/4 and the dashed curve y = x²/2, twice as tall at every x. The shaded region under the dashed curve from 0 to 2 has area 4/3, twice the 2/3 under the gold one.

A sum splits

At each x the height of f + g is the height of f plus the height of g, so each strip (f(xᵢ) + g(xᵢ)) Δx is f(xᵢ) Δx + g(xᵢ) Δx. Adding up the strips, ∫ (f + g) dx = ∫ f dx + ∫ g dx.

Check it from 0 to 2 with f(x) = x² and g(x) = 2x. An antiderivative of x² + 2x is x³/3 + x², which gives 8/3 + 4 = 20/3. Separately, x² gives 8/3 and 2x gives 2² = 4, and 8/3 + 4 = 20/3.

A product does not split. From 0 to 1, the integral of x × x = x² is 1/3, but the integral of x is ½, and ½ × ½ = ¼.

Joining two intervals

The integral from a to b plus the integral from b to c is (F(b) − F(a)) + (F(c) − F(b)) = F(c) − F(a), the integral from a to c. The F(b) cancels.

On y = x²/4: from 0 to 2 the integral is 2/3, from 2 to 4 it is 64/12 − 8/12 = 14/3, and 2/3 + 14/3 = 16/3, which is 64/12, the integral from 0 to 4.

The point in the middle need not lie between the other two, once a reversed integral counts negative. From 0 to 6 the integral is 216/12 = 18, and from 6 to 4 it is −(18 − 16/3) = −38/3. Together they give 18 − 38/3 = 16/3, the integral from 0 to 4 again.

xyabc

The region under y = x²/4 from a = 0 to c = 4, with b = 2 marked on the axis. The part from a to b has area 2/3 and the part from b to c has area 14/3; together they make 16/3.

The usual mistakes

Keeping the sign when the limits are swapped. If the integral from 2 to 5 is 7, the integral from 5 to 2 is −7, not 7.

Giving f(3) for the integral from 3 to 3. A height times no width is 0.

Adding the constant instead of multiplying by it. The integral of 5f(x) is 5 times the integral of f(x), not the integral of f(x) plus 5.

Splitting a product as if it were a sum. From 0 to 1, x × x integrates to 1/3, not to ½ × ½.

Multiplying or subtracting the pieces of a joined interval. If 0 to 2 gives 3 and 2 to 5 gives 4, then 0 to 5 gives 3 + 4 = 7.

A boiler’s gas

In the application below, the gas burnt over a morning is split at a change of tariff. The two pieces add back to the whole, and reading the last stretch backwards gives the same amount with its sign changed.

Worked example: A District Heating Boiler's Gas: A Total Read Off an Antiderivative Rather Than Summed

Question A district heating boiler burns gas at g = 3h2 + 8h + 5 cubic meters per hour, where h is the number of hours after 6:00. (a) How much gas does it burn between 6:00 and noon? (b) The tariff changes at 10:00. How much gas is burnt on each side of that change, and do the two parts add back to the whole?

  1. 1.The gas burnt between 6:00 and noon is ∫06(3h2 + 8h + 5)dh. Rather than add up slivers, find one antiderivative G of the rate; the theorem then gives the area as G(6) − G(0).

    0501001500246h, hours after 6:00cubic meters per hourgas burnt = the area under the rate curve
    0501001500246h, hours after 6:00cubic meters per hourgas burnt = the area under the rate curve
    The gas burnt is ∫06(3h2 + 8h + 5)dh, the area under the rate curve.
  2. 2.Integrating term by term, G(h) = h3 + 4h2 + 5h. Any constant may be added to G, but it cancels in the difference, so take the constant to be zero.

    0501001500246h, hours after 6:00cubic meters per hourgas burnt = the area under the rate curveG(h) = h3+ 4h2+ 5h
    0501001500246h, hours after 6:00cubic meters per hourgas burnt = the area under the rate curveG(h) = h3+ 4h2+ 5h
    One antiderivative is G(h) = h3 + 4h2 + 5h; the theorem asks only for G(6) − G(0).
  3. 3.(a) G(6) = 216 + 144 + 30 = 390 and G(0) = 0, so the boiler burns 390 − 0 = 390 cubic meters between 6:00 and noon.

    0501001500246h, hours after 6:00cubic meters per hour390 m3gas burnt = the area under the rate curveG(h) = h3+ 4h2+ 5h(a) G(6) − G(0) = 390 − 0 = 390
    0501001500246h, hours after 6:00cubic meters per hour390 m3gas burnt = the area under the rate curveG(h) = h3+ 4h2+ 5h(a) G(6) − G(0) = 390 − 0 = 390
    (a) G(6) = 216 + 144 + 30 = 390, so the boiler burns 390 cubic meters between 6:00 and noon.
  4. 4.The tariff changes at h = 4. There G(4) = 64 + 64 + 20 = 148, so the gas burnt before 10:00 is G(4) − G(0) = 148 cubic meters.

    0501001500246h, hours after 6:00cubic meters per hour148 m3gas burnt = the area under the rate curveG(h) = h3+ 4h2+ 5h(a) G(6) − G(0) = 390 − 0 = 390G(4) = 64 + 64 + 20 = 148
    0501001500246h, hours after 6:00cubic meters per hour148 m3gas burnt = the area under the rate curveG(h) = h3+ 4h2+ 5h(a) G(6) − G(0) = 390 − 0 = 390G(4) = 64 + 64 + 20 = 148
    The tariff changes at h = 4, where G(4) = 148: that is the gas burnt before 10:00.
  5. 5.(b) After 10:00 the gas burnt is ∫46 g dh = G(6) − G(4) = 390 − 148 = 242 cubic meters. Check: 148 + 242 = 390, the whole, which is the rule that ∫04 and ∫46 together make ∫06. Reading that last stretch backwards would give ∫64 g dh = −242, the same size with its sign turned round.

    0501001500246h, hours after 6:00cubic meters per hour148 m3242 m3gas burnt = the area under the rate curveG(h) = h3+ 4h2+ 5h(a) G(6) − G(0) = 390 − 0 = 390G(4) = 64 + 64 + 20 = 148(b) G(6) − G(4) = 390 − 148 = 242and 148 + 242 = 390, the whole
    0501001500246h, hours after 6:00cubic meters per hour148 m3242 m3gas burnt = the area under the rate curveG(h) = h3+ 4h2+ 5h(a) G(6) − G(0) = 390 − 0 = 390G(4) = 64 + 64 + 20 = 148(b) G(6) − G(4) = 390 − 148 = 242and 148 + 242 = 390, the whole
    (b) After 10:00 the boiler burns G(6) − G(4) = 242 cubic meters, and 148 + 242 = 390.

Answer: (a) 390 cubic meters; (b) 148 cubic meters before 10:00 and 242 after, and 148 + 242 = 390

Common mistakes

  • Working out G(6) and calling it the answer. That is right here only because G(0) happens to be 0; had the antiderivative been written h3 + 4h2 + 5h + 100, the same slip would have given 490. The theorem asks for a difference of two values, never for one value on its own.
  • Splitting the morning at 10:00 and then integrating the later stretch from 0 to 2 because it lasts two hours. The rate depends on the hour of the morning, not on how long the stretch lasts: ∫02 g dh = 8 + 16 + 10 = 34 cubic meters, nothing like the 242 actually burnt between 10:00 and noon.

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