In short

The area under a curve y = f(x) from x = a to x = b (above the x-axis) is the definite integral \int_a^b f(x)\,dx. You compute it by slicing the region into thin vertical (or horizontal) strips, adding their areas, and taking the limit as the strips become infinitely thin. When the curve dips below the axis, the integral gives a negative contribution — so "area" requires taking absolute values of the pieces.

A farmer owns a rectangular plot, 100 metres long and 40 metres wide. Its area is 100 \times 40 = 4000 square metres. That computation takes one multiplication.

Now suppose the plot is not rectangular. One edge follows a river, and the river curves. The plot is still 100 metres long, but the width changes at every point — it might be 40 metres wide at one end, 55 metres in the middle, and 30 metres at the other end. What is the area now?

There is no single width to multiply by. The shape has no formula from elementary geometry. You need a new idea.

The idea is simple: slice the region into thin vertical strips. Each strip is so thin that the curve barely changes across it, so each strip is approximately a rectangle. Add up the areas of all those thin rectangles. The thinner you make them, the closer the sum gets to the true area. The exact area is the limit of this sum — and that limit is exactly what a definite integral computes.

This is the connection between integration and area: the definite integral is a machine for adding up infinitely many infinitely thin strips.

Building the picture with strips

Take a concrete curve: y = x^2 from x = 0 to x = 3. The region you want is everything below the parabola and above the x-axis, between x = 0 and x = 3.

Slice this region into n vertical strips, each of width \Delta x = 3/n. The k-th strip sits at position x_k = k \cdot \Delta x and has height approximately f(x_k) = x_k^2. Its area is roughly x_k^2 \cdot \Delta x.

The total area is approximately

S_n = \sum_{k=1}^{n} x_k^2 \cdot \Delta x = \sum_{k=1}^{n} \left(\frac{3k}{n}\right)^2 \cdot \frac{3}{n} = \frac{27}{n^3} \sum_{k=1}^{n} k^2

Using the standard formula \sum_{k=1}^{n} k^2 = \frac{n(n+1)(2n+1)}{6}:

S_n = \frac{27}{n^3} \cdot \frac{n(n+1)(2n+1)}{6} = \frac{27(n+1)(2n+1)}{6n^2}

Try a few values. With n = 4 strips: S_4 = \frac{27 \cdot 5 \cdot 9}{6 \cdot 16} = \frac{1215}{96} = 12.656. With n = 10: S_{10} = \frac{27 \cdot 11 \cdot 21}{600} = \frac{6237}{600} = 10.395. With n = 100: S_{100} = \frac{27 \cdot 101 \cdot 201}{60000} = \frac{548127}{60000} = 9.1355.

The numbers are settling toward something. As n \to \infty:

\lim_{n \to \infty} S_n = \lim_{n \to \infty} \frac{27(n+1)(2n+1)}{6n^2} = \frac{27 \cdot 2}{6} = 9

The exact area under y = x^2 from 0 to 3 is 9 square units.

The parabola $y = x^2$ from $x = 0$ to $x = 3$. The vertical lines suggest the strip-slicing idea: each strip is nearly a rectangle, and the sum of their areas approaches the true area (9 square units) as the strips become thinner.

The formal definition

What you just computed — the limit of a sum of strip areas — is exactly the definite integral. Here is the precise statement.

Area below a curve and above the x-axis

If f(x) \geq 0 on the interval [a, b], the area of the region bounded by y = f(x), the x-axis, and the vertical lines x = a and x = b is

A = \int_a^b f(x)\,dx

This is the definite integral of f from a to b.

Reading the definition. The integral sign \int is a stretched-out S — it stands for "sum." The dx at the end represents the width of each infinitesimal strip. The expression f(x)\,dx is the area of one strip: height times width. The integral adds up all these strip-areas from x = a to x = b.

To actually compute the integral, you find an antiderivative F(x) — a function whose derivative is f(x) — and evaluate:

\int_a^b f(x)\,dx = F(b) - F(a)

This is the Fundamental Theorem of Calculus at work. For f(x) = x^2, the antiderivative is F(x) = x^3/3, so

\int_0^3 x^2\,dx = \frac{3^3}{3} - \frac{0^3}{3} = 9 - 0 = 9

Exactly what the limit-of-sums approach gave.

Vertical strips vs. horizontal strips

So far, every strip has been vertical: a thin rectangle standing upright, with its base on the x-axis and its top touching the curve. This is the natural approach when the curve is written as y = f(x).

But sometimes the curve is easier to describe as x = g(y) — a function of y. In that case, horizontal strips are the natural choice.

A horizontal strip lies on its side. Its "base" is on the y-axis, and it extends rightward to the curve x = g(y). Its height is a thin slice dy, and its width is g(y). The area of one horizontal strip is g(y)\,dy, and the total area is

A = \int_{y_1}^{y_2} g(y)\,dy

where y_1 and y_2 are the y-values at the bottom and top of the region.

When to use which. Use vertical strips when the curve is naturally y = f(x). Use horizontal strips when the curve is naturally x = g(y), or when vertical strips would force you to split the region into multiple pieces. Both methods give the same answer — you are just slicing the same region in different directions.

Take the parabola x = y^2 from y = 0 to y = 2. Using horizontal strips, the area between the curve and the y-axis is

A = \int_0^2 y^2\,dy = \frac{y^3}{3}\Big|_0^2 = \frac{8}{3}

If you tried vertical strips here, you would need to rewrite the curve as y = \sqrt{x} and integrate from x = 0 to x = 4: \int_0^4 \sqrt{x}\,dx = \frac{2}{3}x^{3/2}\big|_0^4 = \frac{2}{3}(8) = \frac{16}{3}. But that gives the area under y = \sqrt{x} above the x-axis — which is the region above the parabola inside the rectangle [0,4] \times [0,2]. The area below the parabola (between the curve and the y-axis) is the rectangle's area minus this: 4 \times 2 - 16/3 = 24/3 - 16/3 = 8/3. Both approaches agree.

Signed area: what happens below the axis

There is an important subtlety. The definite integral \int_a^b f(x)\,dx does not always give you "area" in the geometric sense. When the curve dips below the x-axis, the integral subtracts the contribution from the below-axis region instead of adding it.

Take f(x) = x^2 - 4 on the interval [0, 3]. This parabola sits below the x-axis between x = 0 and x = 2 (since x^2 - 4 < 0 there) and above the axis from x = 2 to x = 3.

If you blindly compute the integral:

\int_0^3 (x^2 - 4)\,dx = \left[\frac{x^3}{3} - 4x\right]_0^3 = (9 - 12) - 0 = -3

A negative answer — which cannot be a geometric area. What happened? The below-axis piece contributed -16/3 and the above-axis piece contributed 7/3, and the integral added them with their signs: -16/3 + 7/3 = -3.

To find the actual geometric area, you must handle the below-axis and above-axis parts separately, taking the absolute value of each:

A = \int_0^2 |x^2 - 4|\,dx + \int_2^3 (x^2 - 4)\,dx = \int_0^2 (4 - x^2)\,dx + \int_2^3 (x^2 - 4)\,dx
= \left[4x - \frac{x^3}{3}\right]_0^2 + \left[\frac{x^3}{3} - 4x\right]_2^3 = \left(8 - \frac{8}{3}\right) + \left(-3 - \left(-\frac{16}{3}\right)\right) = \frac{16}{3} + \frac{7}{3} = \frac{23}{3}

The geometric area is 23/3, not -3. The rule is: find where the curve crosses the axis, split the integral at those points, and take the absolute value of each piece.

The parabola $y = x^2 - 4$. Between $x = 0$ and $x = 2$ the curve lies below the $x$-axis, giving a negative integral contribution. Between $x = 2$ and $x = 3$ it is above the axis. To find geometric area, you split at $x = 2$ and take absolute values of each piece.

Computing areas: the workflow

Here is the process for finding the area of a region bounded by a curve and the axes.

  1. Sketch the curve. Identify where it crosses the x-axis (set f(x) = 0 and solve).
  2. Determine the interval [a, b] over which you need the area.
  3. Check the sign of f(x) on each sub-interval. If f(x) \geq 0 throughout, integrate directly. If f(x) changes sign, split at the zeros.
  4. Integrate each piece and take absolute values of the below-axis contributions.
  5. Add the pieces to get the total geometric area.

Example 1: Area under a cubic curve

Find the area bounded by y = x^3 - 4x, the x-axis, and the lines x = 0 and x = 3.

Step 1. Find where the curve crosses the x-axis. Set x^3 - 4x = 0, so x(x^2 - 4) = 0, giving x = 0, x = 2, x = -2.

Why: the zeros tell you where the curve switches from above-axis to below-axis (or vice versa). On [0, 3], the relevant zero is x = 2.

Step 2. Check signs. For 0 < x < 2, test x = 1: 1 - 4 = -3 < 0. For 2 < x < 3, test x = 2.5: 15.625 - 10 = 5.625 > 0. So the curve is below the axis on (0, 2) and above on (2, 3).

Why: you need to know where to split the integral and where to negate, so the geometric area comes out positive everywhere.

Step 3. Compute the below-axis part (take absolute value):

\int_0^2 |x^3 - 4x|\,dx = \int_0^2 (4x - x^3)\,dx = \left[2x^2 - \frac{x^4}{4}\right]_0^2 = (8 - 4) - 0 = 4

Why: since x^3 - 4x < 0 on (0, 2), the absolute value flips the sign to 4x - x^3.

Step 4. Compute the above-axis part:

\int_2^3 (x^3 - 4x)\,dx = \left[\frac{x^4}{4} - 2x^2\right]_2^3 = \left(\frac{81}{4} - 18\right) - (4 - 8) = \frac{9}{4} + 4 = \frac{25}{4}

Why: on (2, 3) the curve is positive, so no sign change is needed.

Step 5. Add the pieces: A = 4 + \frac{25}{4} = \frac{16}{4} + \frac{25}{4} = \frac{41}{4}.

Result: The total geometric area is \dfrac{41}{4} square units.

The cubic $y = x^3 - 4x$ on $[0, 3]$. The curve dips below the axis between $x = 0$ and $x = 2$ (contributing area 4), then rises above between $x = 2$ and $x = 3$ (contributing area $25/4$). The total geometric area is $41/4$.

The graph confirms what the algebra told you: two distinct regions, one below and one above the axis, each contributing positively to the total area.

Example 2: Area using horizontal strips

Find the area enclosed between the curve x = 4 - y^2 and the y-axis.

Step 1. Identify the region. The curve x = 4 - y^2 is a parabola opening leftward with vertex at (4, 0). It crosses the y-axis (x = 0) when 4 - y^2 = 0, giving y = -2 and y = 2.

Why: the y-intercepts tell you the vertical extent of the region. The region is bounded on the right by the parabola and on the left by the y-axis.

Step 2. Check that x = 4 - y^2 \geq 0 for -2 \leq y \leq 2. At y = 0, x = 4 > 0. At y = \pm 1, x = 3 > 0. The curve stays to the right of the y-axis throughout. No sign issues.

Why: since x \geq 0 throughout, horizontal strips give positive area directly. No splitting needed.

Step 3. Set up the integral with horizontal strips. Each strip at height y has width g(y) = 4 - y^2 and thickness dy.

A = \int_{-2}^{2} (4 - y^2)\,dy

Why: horizontal strips are natural here because the curve is expressed as x in terms of y.

Step 4. Evaluate.

A = \left[4y - \frac{y^3}{3}\right]_{-2}^{2} = \left(8 - \frac{8}{3}\right) - \left(-8 + \frac{8}{3}\right) = \frac{16}{3} + \frac{16}{3} = \frac{32}{3}

Why: the function 4 - y^2 is symmetric about y = 0, so the integral from -2 to 2 is twice the integral from 0 to 2. The final answer 32/3 matches this: 2 \times 16/3 = 32/3.

Result: The enclosed area is \dfrac{32}{3} square units.

The sideways parabola $x = 4 - y^2$. The shaded region between the curve and the $y$-axis has area $32/3$. Horizontal strips are the natural choice here — each strip runs from $x = 0$ to $x = 4 - y^2$.

The picture shows a symmetric region: the parabola opens to the left, and the enclosed area bulges out from the y-axis. The 32/3 \approx 10.67 square units fits — the region is roughly an oval about 4 units wide and 4 units tall, so its area should be somewhat less than 4 \times 4 = 16, and 32/3 is exactly that.

Common confusions

Going deeper

If you came here to understand how integration gives area, you have it — you can stop here. The rest of this section explores the Riemann sum more carefully, the formal connection to limits, and a few boundary cases.

Left sums, right sums, and the squeeze

In the strip computation above, you used right endpoints: each strip's height was f(x_k) where x_k is the right edge of the strip. You could equally have used the left edge, giving a left Riemann sum. For an increasing function, the left sum underestimates and the right sum overestimates. For a decreasing function, it is reversed.

The key fact is: as n \to \infty, both the left and right sums converge to the same number — the definite integral. This is not obvious, and the proof uses the fact that continuous functions on closed intervals are uniformly continuous. The result is that you can use any point within each strip (left endpoint, right endpoint, midpoint, or any other choice) and the limit is the same.

Area as the antiderivative's increment

Why does the Fundamental Theorem of Calculus work? Define A(x) = \int_a^x f(t)\,dt — the area under the curve from a to a variable right endpoint x. When you move the right endpoint by a tiny amount h, the area increases by approximately f(x) \cdot h (one more thin strip). So A'(x) = f(x) — the rate at which area accumulates is the height of the curve. That means A(x) is an antiderivative of f(x), and the total area from a to b is A(b) - A(a) = F(b) - F(a) for any antiderivative F.

This is the deep reason integration and differentiation are reverse operations: differentiation measures rates, and integration accumulates. The area function is the bridge between them.

Curves that touch the axis

When f(x) = 0 at a single point but does not change sign, no splitting is needed — the integral is still positive. For example, y = (x-1)^2 touches the axis at x = 1 but never goes below it. The integral \int_0^2 (x-1)^2\,dx = 2/3 is the correct geometric area without any adjustments.

The splitting rule applies only when f actually changes sign — when it crosses from positive to negative or vice versa.

Where this leads next

You now know how to find the area of a region bounded by a single curve and the axes. The next set of articles extends this to more complex regions.