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The definite integral abf(x)dx\int_{a}^{b} f(x) \, dx measures the signed area between the curve f(x)f(x) and the x-axis from x=ax = a to x=bx = b. The concept arises from Riemann sums: dividing the interval [a,b][a, b] into nn subintervals, forming rectangles of width Δx\Delta x and height f(xi)f(x_i), and summing all their areas. As nn \to \infty and Δx0\Delta x \to 0, this sum converges to the exact integral.

Regions where f(x)f(x) is negative contribute negative area to the definite integral.

The Fundamental Theorem of Calculus (FTC) connects differentiation and integration. Part 1 states that if FF is the antiderivative of ff, then ddx[f(t)dt from a to x]=f(x)\frac{d}{dx}\left[\int f(t) \, dt \text{ from } a \text{ to } x\right] = f(x). Part 2 provides the evaluation shortcut: abf(x)dx=F(b)F(a)\int_{a}^{b} f(x) \, dx = F(b) - F(a), where FF is any antiderivative of ff.

Integration also computes displacement, net change, work, and probability - any quantity that accumulates continuously over a continuous variable. The indefinite integral f(x)dx=F(x)+C\int f(x) \, dx = F(x) + C finds families of antiderivatives, with the constant CC representing the entire family.

Understanding Integral as Area

Riemann sums are more than a drawing method. Each rectangle estimates what happens over a short interval. A left endpoint choice can place every height too low on an increasing graph, while a right endpoint choice places them too high.

Midpoint rectangles often reduce the error because they sample nearer the center. The key point is not that one sum is exact. Upper and lower estimates can squeeze toward one value as the intervals become smaller.

Smooth graphs usually behave well. A function with jumps, sharp breaks, or infinite values needs more care. Some functions cannot be handled by ordinary Riemann sums.

An integral has units, and those units tell you what the result means. If velocity is measured in metres per second and time is measured in seconds, integrating velocity over time gives metres. The result is displacement.

If water flows through a pipe in litres per minute, integrating the flow rate over minutes gives litres. This is why integrals appear in utility bills, rainfall records, medicine doses, population models, and physics experiments. The graph may look like an area problem, but the result often represents a total amount rather than a flat physical region.

The Fundamental Theorem works because an accumulation function keeps a running total from a fixed starting point to a moving endpoint. When that endpoint moves a tiny amount, the total changes by about the height of the graph times that tiny width. This makes the rate of change of the accumulated total equal to the original function.

Antiderivatives provide a fast way to calculate a finished total without adding thousands of rectangles. The constant in an indefinite integral does not affect a definite integral because it cancels when the endpoint values are compared.

The order of the endpoints matters. Reading an interval backward changes the sign of the result.

A common mistake is treating net change as the same thing as total change. For velocity, motion in opposite directions cancels in displacement. Total distance requires every part of the trip to count as positive, so the interval must be split where velocity changes sign or the absolute value of velocity must be used.

Students should inspect the graph before calculating. Look for crossings of the horizontal axis, turning points, gaps, and changes in units.

With tables of data, the exact curve may be unknown, so numerical methods such as midpoint or trapezoidal estimates are used. More data points usually help, but rounded data still limits accuracy.

Key Facts

  • Definite integral = signed area under curve; negative where f(x)<0f(x) < 0
  • Riemann sum: f(xi)Δxabf(x)dx\sum f(x_i)\Delta x \to \int_{a}^{b} f(x) \, dx as nn \to \infty
  • FTC Part 2: abf(x)dx=F(b)F(a)\int_{a}^{b} f(x) \, dx = F(b) - F(a), where F(x)=f(x)F'(x) = f(x)
  • Power rule for integration: xndx=xn+1n+1+C\int x^n \, dx = \frac{x^{n+1}}{n+1} + C (n1n \neq -1)
  • abf(x)dx=baf(x)dx\int_{a}^{b} f(x) \, dx = -\int_{b}^{a} f(x) \, dx (reversing limits changes sign)
  • Net displacement ≠ total distance; total distance = ∫|v(t)| dt

Vocabulary

Definite integral
The limit of a Riemann sum giving the signed area under a curve f(x)f(x) between x=ax = a and x=bx = b.
Antiderivative
A function F(x)F(x) whose derivative is f(x)f(x); also called an indefinite integral. Differs from another antiderivative by only a constant CC.
Riemann sum
An approximation of the area under a curve using rectangles; the basis for the definition of the definite integral.
Fundamental Theorem of Calculus
The theorem connecting differentiation and integration: differentiation and integration are inverse operations, and antiderivatives evaluate definite integrals.
Accumulation function
A function of the form A(x)=axf(t)dtA(x) = \int_a^x f(t)\,dt that represents the accumulated area (or net change) from a fixed point aa up to xx.

Common Mistakes to Avoid

  • Forgetting the constant of integration for indefinite integrals. f(x)dx=F(x)+C\int f(x)\,dx = F(x) + C, not just F(x)F(x). The constant matters because it represents an entire family of antiderivatives.
  • Treating negative areas as zero. If f(x)f(x) is negative on part of [a,b][a,b], the integral subtracts that region's area. The definite integral gives net signed area, not total area.
  • Applying the power rule to 1xdx\int \frac{1}{x}\,dx. xndx=xn+1n+1\int x^n\,dx = \frac{x^{n+1}}{n+1} fails when n=1n = -1 (division by zero). Instead, 1xdx=lnx+C\int \frac{1}{x}\,dx = \ln|x| + C.
  • Confusing indefinite and definite integrals. f(x)dx\int f(x)\,dx is a family of functions +C+ C; abf(x)dx\int_a^b f(x)\,dx is a single number (the area). The definite integral needs bounds.

Practice Questions

  1. 1 Evaluate ∫[0 to 3] (x² − 2x) dx. Identify any regions where the integrand is negative and how they affect the result.
  2. 2 Find the total area (not net area) between f(x)=x24f(x) = x^2 - 4 and the xx-axis from x=0x = 0 to x=3x = 3.
  3. 3 A particle moves with velocity v(t)=t24t+3v(t) = t^2 - 4t + 3 m/s. Find the displacement and total distance traveled from t=0t = 0 to t=4t = 4 s.