The area function
Take the curve and shade the region under it from x = 0 up to some point x. Call the shaded area A(x). It is a function of x: move the right edge and the area changes. From area under a curve, , and .
Push the right edge a little further, from x to x + h. The shaded region gains a thin strip, h wide, standing between x and x + h.
The area under from 0 up to x = 2, which is . Moving the right edge to the right adds a strip to the shaded region.
How fast the area grows
The new strip is h wide, and its height is close to f(x), the height of the curve at the edge. So the area grows by about f(x) × h: .
Divide by h. The rate at which the area grows, , is about f(x), and the thinner the strip, the closer its top comes to a flat line at height f(x). As h shrinks to 0 the approximation becomes exact: A'(x) = f(x). The area function differentiates to the curve’s own height.
Check it at x = 2, where f(2) = 4. A strip 0.01 wide adds to the area, and 0.0402003 ÷ 0.01 = 4.02, close to 4.
the sign ∫ is an S for sum: each sliver is height f(x) × width Δx = 0.288, and the integral adds them across the interval
Narrow the sliver to dx = 0.01
A sliver under , starting at x = 1.2, where the height is 1.44. At width the rectangle has area 1.44 × 0.2 = 0.288, against the 0.339 of the strip under the curve. Narrow it to 0.01: the strip becomes a rectangle 1.44 tall, so the area grows at the rate 1.44 at x = 1.2.
Areas from antiderivatives
So A is an antiderivative of f. Now take any antiderivative F of f. A and F have the same derivative, so their graphs have the same gradient at every x, and one is the other slid up or down: A(x) = F(x) + c for some constant c.
The area from a to a is 0, so 0 = F(a) + c, which gives c = −F(a). Then the area from a to b is A(b) = F(b) − F(a). This is the fundamental theorem of calculus: the integral from a to b of f(x) dx is F(b) − F(a), for any antiderivative F. It is written .
Any antiderivative gives the same answer, because the constant cancels. With , the area under from 1 to 3 is , the same as with .
Check by strips: 1000 midpoint rectangles from 1 to 3 add to 8.666666, within a millionth of it.
An area that is a triangle
The region under y = 2x from 0 to 3 is a triangle with base 3 and height 6, so its area is ½ × 3 × 6 = 9. An antiderivative of 2x is , and . In general the integral of 2x from 0 to b is .
The region under y = 2x from 0 to 3: a triangle with base 3 and height 6, area 9, which is .
The usual mistakes
Giving the height in place of the area. For y = 2x from 0 to 3, 6 is the height at x = 3; the area is 9.
Giving the width. 3 is the length of the interval from 0 to 3, not the area over it.
Using F(b) alone. That works only when F(a) = 0: the area under from 1 to 3 is , not 9.
Subtracting the wrong way round. F(a) − F(b) gives for the area under from 1 to 3.
A boiler’s gas
In the application below, a boiler burns gas at a rate that changes through the morning. The gas burnt is the area under the rate curve, read off one antiderivative as a difference of two values, then split at a change of tariff.
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.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).
The gas burnt is ∫06(3h2 + 8h + 5)dh, the area under the rate curve. 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.
One antiderivative is G(h) = h3 + 4h2 + 5h; the theorem asks only for G(6) − G(0). 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.
(a) G(6) = 216 + 144 + 30 = 390, so the boiler burns 390 cubic meters between 6:00 and noon. 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.
The tariff changes at h = 4, where G(4) = 148: that is the gas burnt before 10:00. 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.
(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.
More techniques of integration problems, worked step by step →