Chapter 2 Proofs: Theorems on Definite Integrals
This page provides rigorous proofs of the key theorems stated on the Definite Integral page. Each proof uses fundamental tools of analysis such as the definition of Riemann sums and the Mean Value Theorem.
Fundamental Theorem of Calculus (First Form)
Theorem. If $f$ is continuous on the closed interval $[a,b]$ and $F$ is an antiderivative of $f$ (i.e., $F'(x) = f(x)$), then
$$\int_a^b f(x)\,dx = F(b) - F(a)$$Proof.
Let $P = \{a = x_0 < x_1 < \cdots < x_n = b\}$ be an arbitrary partition of $[a,b]$. By the telescoping sum we have
$$F(b) - F(a) = \sum_{i=1}^{n} \bigl[F(x_i) - F(x_{i-1})\bigr]$$Applying the Mean Value Theorem to each subinterval $[x_{i-1}, x_i]$, there exists $c_i \in (x_{i-1}, x_i)$ such that
$$F(x_i) - F(x_{i-1}) = F'(c_i)(x_i - x_{i-1}) = f(c_i)\,\Delta x_i$$Therefore
$$F(b) - F(a) = \sum_{i=1}^{n} f(c_i)\,\Delta x_i$$The right-hand side is a Riemann sum. Since $f$ is continuous on $[a,b]$, it is integrable, and as the mesh $\|P\| = \max_i \Delta x_i \to 0$, every Riemann sum converges to $\displaystyle\int_a^b f(x)\,dx$. Since the left-hand side $F(b) - F(a)$ is a constant independent of the partition,
$$F(b) - F(a) = \int_a^b f(x)\,dx$$as required. $\blacksquare$
Fundamental Theorem of Calculus (Second Form)
Theorem. If $f$ is continuous on the closed interval $[a,b]$, then the function
$$G(x) = \int_a^x f(t)\,dt$$is differentiable on $[a,b]$ and $G'(x) = f(x)$.
Proof.
Fix $x \in [a,b]$ and consider the difference quotient for $h \neq 0$ (with $x+h \in [a,b]$).
$$\frac{G(x+h) - G(x)}{h} = \frac{1}{h}\left[\int_a^{x+h} f(t)\,dt - \int_a^x f(t)\,dt\right] = \frac{1}{h}\int_x^{x+h} f(t)\,dt$$Since $f$ is continuous on a closed interval, by the Mean Value Theorem for integrals there exists $c_h$ between $x$ and $x+h$ such that
$$\frac{1}{h}\int_x^{x+h} f(t)\,dt = f(c_h)$$As $h \to 0$, we have $c_h \to x$, and by the continuity of $f$, $f(c_h) \to f(x)$. Therefore
$$G'(x) = \lim_{h \to 0} \frac{G(x+h) - G(x)}{h} = \lim_{h \to 0} f(c_h) = f(x)$$as required. $\blacksquare$
Linearity of Definite Integrals
Theorem. If $f, g$ are Riemann integrable on $[a,b]$ and $\alpha, \beta$ are constants, then
$$\int_a^b \bigl[\alpha\,f(x) + \beta\,g(x)\bigr]\,dx = \alpha\int_a^b f(x)\,dx + \beta\int_a^b g(x)\,dx$$Proof.
For any partition $P = \{x_0, x_1, \dots, x_n\}$ of $[a,b]$ and sample points $\xi_i \in [x_{i-1}, x_i]$, consider the Riemann sum.
$$\sum_{i=1}^{n} \bigl[\alpha\,f(\xi_i) + \beta\,g(\xi_i)\bigr]\,\Delta x_i = \alpha \sum_{i=1}^{n} f(\xi_i)\,\Delta x_i + \beta \sum_{i=1}^{n} g(\xi_i)\,\Delta x_i$$This holds trivially by the linearity of finite sums. Taking the limit as $\|P\| \to 0$, since both $f$ and $g$ are integrable, each Riemann sum converges to the respective definite integral. Therefore
$$\int_a^b \bigl[\alpha\,f(x) + \beta\,g(x)\bigr]\,dx = \alpha\int_a^b f(x)\,dx + \beta\int_a^b g(x)\,dx$$as required. $\blacksquare$
Interval Splitting
Theorem. If $f$ is Riemann integrable on $[a,b]$ and $a < c < b$, then
$$\int_a^b f(x)\,dx = \int_a^c f(x)\,dx + \int_c^b f(x)\,dx$$Proof.
Consider a partition $P$ of $[a,b]$ that includes $c$ as a partition point (say $c = x_k$). Then
$$P_1 = \{x_0, x_1, \dots, x_k\}, \quad P_2 = \{x_k, x_{k+1}, \dots, x_n\}$$are partitions of $[a,c]$ and $[c,b]$ respectively, and the Riemann sum with sample points $\xi_i$ decomposes as
$$\sum_{i=1}^{n} f(\xi_i)\,\Delta x_i = \sum_{i=1}^{k} f(\xi_i)\,\Delta x_i + \sum_{i=k+1}^{n} f(\xi_i)\,\Delta x_i$$For a partition that does not include $c$, we can consider the refinement obtained by adding $c$. The Riemann sum changes by at most $2M\|P\|$ (where $M = \sup|f|$), which vanishes as $\|P\| \to 0$.
Therefore, taking the limit as $\|P\| \to 0$,
$$\int_a^b f(x)\,dx = \int_a^c f(x)\,dx + \int_c^b f(x)\,dx$$as required. $\blacksquare$
Endpoint Swap
Theorem. If $f$ is Riemann integrable on $[a,b]$, then
$$\int_b^a f(x)\,dx = -\int_a^b f(x)\,dx$$Proof.
For $a < b$, the definite integral is defined as the limit of Riemann sums:
$$\int_a^b f(x)\,dx = \lim_{\|P\| \to 0} \sum_{i=1}^{n} f(\xi_i)\,(x_i - x_{i-1})$$When $a > b$, the integral is defined by taking a partition $b = x_0 < x_1 < \cdots < x_n = a$ as a Riemann sum. Here $\Delta x_i = x_i - x_{i-1} > 0$, but the direction from $a$ to $b$ is reversed, so by convention
$$\int_b^a f(x)\,dx := -\int_a^b f(x)\,dx$$This can also be derived from the interval splitting property. Setting $c = a$ in the interval splitting theorem gives
$$\int_a^a f(x)\,dx = \int_a^b f(x)\,dx + \int_b^a f(x)\,dx$$Since the left-hand side is $0$ (proved in the next section),
$$\int_b^a f(x)\,dx = -\int_a^b f(x)\,dx$$as required. $\blacksquare$
Same Endpoint
Theorem. For any $a$ and any function $f$ integrable at $a$,
$$\int_a^a f(x)\,dx = 0$$Proof.
Since the length of the integration interval is $0$, for any partition $P$ the interval $[a,a]$ consists only of $\Delta x_i = 0$. Therefore the Riemann sum is
$$\sum_{i=1}^{n} f(\xi_i)\,\Delta x_i = 0$$Since every Riemann sum equals $0$, the limit is also $0$.
$$\int_a^a f(x)\,dx = 0$$$\blacksquare$
Inequality
Theorem. If $f, g$ are Riemann integrable on $[a,b]$ and $f(x) \le g(x)$ for all $x \in [a,b]$, then
$$\int_a^b f(x)\,dx \le \int_a^b g(x)\,dx$$Proof.
Define $h(x) = g(x) - f(x)$. By hypothesis, $h(x) \ge 0$ for all $x \in [a,b]$. Since $h$ is the difference of two integrable functions, it is integrable.
For any partition $P$ and sample points $\xi_i$, since $h(\xi_i) \ge 0$ and $\Delta x_i > 0$,
$$\sum_{i=1}^{n} h(\xi_i)\,\Delta x_i \ge 0$$Taking the limit as $\|P\| \to 0$,
$$\int_a^b h(x)\,dx \ge 0$$By linearity,
$$\int_a^b g(x)\,dx - \int_a^b f(x)\,dx \ge 0$$That is, $\displaystyle\int_a^b f(x)\,dx \le \int_a^b g(x)\,dx$. $\blacksquare$
Even and Odd Functions
Theorem. If $f$ is Riemann integrable on $[-a, a]$, then
- If $f$ is even ($f(-x) = f(x)$), then $\displaystyle\int_{-a}^{a} f(x)\,dx = 2\int_0^a f(x)\,dx$
- If $f$ is odd ($f(-x) = -f(x)$), then $\displaystyle\int_{-a}^{a} f(x)\,dx = 0$
Proof.
By the interval splitting property,
$$\int_{-a}^{a} f(x)\,dx = \int_{-a}^{0} f(x)\,dx + \int_0^a f(x)\,dx$$Apply the substitution $x = -t$ ($dx = -dt$) to the left integral. When $x = -a$ we have $t = a$, and when $x = 0$ we have $t = 0$, so
$$\int_{-a}^{0} f(x)\,dx = \int_a^0 f(-t)\,(-dt) = \int_0^a f(-t)\,dt$$Therefore
$$\int_{-a}^{a} f(x)\,dx = \int_0^a f(-t)\,dt + \int_0^a f(x)\,dx = \int_0^a \bigl[f(-x) + f(x)\bigr]\,dx$$(1) Even function case: Since $f(-x) = f(x)$,
$$\int_{-a}^{a} f(x)\,dx = \int_0^a \bigl[f(x) + f(x)\bigr]\,dx = 2\int_0^a f(x)\,dx$$(2) Odd function case: Since $f(-x) = -f(x)$,
$$\int_{-a}^{a} f(x)\,dx = \int_0^a \bigl[-f(x) + f(x)\bigr]\,dx = \int_0^a 0\,dx = 0$$$\blacksquare$
Related Topics
- Chapter 2: Definite Integral — theorem statements and worked examples
- Chapter 1 Proofs: Fundamental Formulas of Indefinite Integrals
- Chapter 3: Integration by Substitution