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Physics · Ch 2 — Mathematical Methods

Integral calculus

2.6.2

Integral calculus

Integral calculus deals with the properties and applications of integrals. Physically, the integral of a function f(x)f(x), written ∫f(x) dx\int f(x)\,dx, represents the AREA under the curve of f(x)f(x) plotted against xx. Integration is the reverse process of differentiation.

Motivating the definite integral. For simple shapes (a rectangle, a triangle) the area under a straight-line graph between x=ax=a and x=bx=b can be found directly — e.g. as the sum of a rectangle of area f(a)(b−a)f(a)(b-a) and a triangle of area 12(b−a)(f(b)−f(a))\tfrac12(b-a)\big(f(b)-f(a)\big). For a general curve, no such simple formula exists, so the area is approximated by dividing the region into a large number nn of thin vertical strips, each treated as a rectangle, and summing their areas:

Area≈∑i=1n(xi−xi−1)f(xi)\text{Area} \approx \sum_{i=1}^{n}(x_i-x_{i-1})f(x_i)

As n→∞n\to\infty (each strip becomes infinitesimally thin), this sum converges to the EXACT area under the curve:

Area=lim⁡n→∞∑i=1n(xi−xi−1)f(xi)— (2.40)\text{Area} = \lim_{n\to\infty}\sum_{i=1}^{n}(x_i-x_{i-1})f(x_i) \qquad \text{--- (2.40)}

This limiting sum, from x=ax=a to x=bx=b, is called the definite integral of f(x)f(x) and is written

∫x=ax=bf(x) dx— (2.41)\int_{x=a}^{x=b} f(x)\,dx \qquad \text{--- (2.41)}

Indefinite integral and the link to differentiation. F(x)=∫f(x) dxF(x) = \int f(x)\,dx --- (2.42) is called the indefinite integral of f(x)f(x) (no limits on xx). Since integration reverses differentiation, f(x)=ddx(F(x))f(x) = \dfrac{d}{dx}\big(F(x)\big) --- (2.43), and the definite integral is evaluated as

[F(x)]ab=F(b)−F(a)=∫abf(x) dx— (2.44)\Big[F(x)\Big]_a^b = F(b)-F(a) = \int_a^b f(x)\,dx \qquad \text{--- (2.44)}

Properties of integration.

  1. ∫(f1(x)+f2(x)) dx=∫f1(x) dx+∫f2(x) dx\int\big(f_1(x)+f_2(x)\big)\,dx = \int f_1(x)\,dx+\int f_2(x)\,dx --- (2.45)
  2. ∫Kf(x) dx=K∫f(x) dx\int K f(x)\,dx = K\int f(x)\,dx, for K=K= constant --- (2.46)

Standard indefinite integrals.

∫xn dx=xn+1n+1— (2.47)∫1x dx=ln⁡x— (2.48)\int x^n\,dx = \dfrac{x^{n+1}}{n+1} \quad \text{--- (2.47)} \qquad \int \dfrac1x\,dx = \ln x \quad \text{--- (2.48)} …

Figure 2.13Area under a straight line and a curve

What this figure shows. Two-panel graph of y=f(x)y=f(x) against xx. Panel (a) shows a STRAIGHT-LINE graph of f(x)f(x) with two points A and B on it (at x=a and x=b), and the region under the line between x=a and x=b shaded — this shaded area is shown decomposed into a rectangle (labelled ADEC, of height f(a) and width b−a) plus a right triangle (labelled ABC, of area 12(b−a)(f(b)−f(a))\tfrac12(b-a)(f(b)-f(a))) sitting on top of it. Panel (b) shows a general CURVED graph of f(x)f(x) (not a straight line), with the area under the curve between two x-values divided into a series of narrow vertical strips of equal small width, each strip drawn as an approximating rectangle whose height touches the curve — illustrating the Riemann-sum method of approximating the area u …

Misc Ex.2.11Evaluating definite and indefinite integrals

Worked out. Three short sub-parts, each asking for the integral of a given function: (a) the indefinite integral ∫x8 dx\int x^8\,dx, a pure power function; (b) the DEFINITE integral ∫25x2 dx\int_2^5 x^2\,dx, evaluated between the limits x=2 and x=5; (c) the indefinite integral of a SUM, ∫(x2+sin⁡x) dx\int(x^2+\sin x)\,dx. The method applies, respectively, the basic power-rule integral ∫xn dx=xn+1/(n+1)\int x^n\,dx = x^{n+1}/(n+1) for (a); the same power-rule formula together with evaluating at the upper and lower limits for (b); and the sum-rule property of integration combined with the standard power and sine integral formulas for (c) — walking through the integration rules in increasing complexity, mirroring the struct …