1. The variable \(x\) that appears in definite integrals is called the dummy variable and we can replace this with another to get the same result:
\(
int_a^b f(x) mathrm{d} x=int_a^b f(t) mathrm{d} t .
\)
Proof:
\(Thus LHS = RHS
2. The definite integral of a constant \(c in mathbf{R}\) is proportional to the width of the interval:
\(int_a^b c mathrm{~d} x=c(b-a)\)
Proof:
\(3. The zero-width limit when \(b=a\) implies that
\(
int_a^a f(x) mathrm{d} x=0 .
\)
Example 1:
\(4. We can interchange the limits on any definite integral using
\(
int_a^b f(x) mathrm{d} x=-int_b^a f(x) mathrm{d} x .
\)
Proof:
\(LHS = RHS
5. We can split up definite integrals with a sum or difference:
\(
int_a^b(f(x) pm g(x)) mathrm{d} x=int_a^b f(x) mathrm{d} x pm int_a^b g(x) mathrm{d} x
\)
Example 2: Integral of Sum of functions: Evaluate the integral \(intleft[x+e^xright] d x\)
According to the above property
\(int_a^b(f(x) + g(x)) mathrm{d} x=int_a^b f(x) mathrm{d} x + int_a^b g(x) mathrm{d} x \\) \(
Proof: Integral of difference of functions
Evaluate the integral
\(
int[2-1 / x] d x
\)
\(
int[2-1 / x] d x=int 2 d x-int(1 / x) d x
\)
\(
=2 x-ln |x|+c
\)
6. We can factor out a constant \(c in mathbf{R}\) from definite integrals:
\(int_a^b c f(x) mathrm{d} x=c int_a^b f(x) mathrm{d} x .\)
Example 3:
\(int_1^2 5 f(x) mathrm{d} x=5 int_1^2 f(x) mathrm{d} x . \)
7. We can also split up the integral with the limits \([a, b]\) for some value \(c in mathbf{R}\) over two adjacent intervals \([a, c]\) and \([c, b]\):
\(
int_a^b f(x) mathrm{d} x=int_a^c f(x) mathrm{d} x+int_c^b f(x) mathrm{d} x .
\)
Example 4:
\(We know that
\(
8. If \(f(x) geq 0\), then \(int_a^b f(x) mathrm{d} x geq 0\)
Example 5:
In this example \(f(x)\) = 4 \(x\), As \(f(x) geq 0 \) its integral is also \(int_1^2 4 x d x geq 0 \)
\(9. If \(f(x) geq g(x)\), then \(int_a^b f(x) mathrm{d} x geq int_a^b g(x) mathrm{d} x .\)
Example 6:
\(
text { Compare } f(x)=sqrt{1+x^2} text { and } g(x)=sqrt{1+x} text { over the interval }[0,1]
\)
Graphing these functions is necessary to understand how they compare over the interval \([0,1]\). Initially, when graphed on a graphing calculator, \(f(x)\) appears to be above \(g(x)\) everywhere. However, on the interval \([0,1]\), the graphs appear to be on top of each other. We need to zoom in to see that, on the interval \([0,1], g(x)\) is above \(f(x)\). The two functions intersect at \(x=0\) and \(x=1\) (as shown in figure a & b).

We can see from the graph that over the interval \([0,1], g(x) geq f(x)\). Comparing the integrals over the specified interval \([0,1]\), we also see that \(int_0^1 g(x) d x geq int_0^1 f(x) d x\) (Figure c & d). The thin, red-shaded area shows just how much difference there is between these two integrals over the interval \([0,1]\).
10. We also have the bounded property; if \(m leq f(x) leq M\), then
\(
m(b-a) leq int_a^b f(x) mathrm{d} x leq M(b-a)
\)
Example 7:
Suppose that on \([-2,5]\), the values of \(f\) lie in the interval \([m, M]\). Between which bounds does \(int_{-2}^5 f(x) mathrm{d} x\) lie?
In this example, we want to find the bounds of an integral using the property where the values of \(f\) lie in a particular interval.
In particular, the following property states that if \(m leq f(x) leq M\), then
\(
m(b-a) leq int_a^b f(x) mathrm{d} x leq M(b-a)
\)
On applying this property with \(a=-2\) and \(b=5\), we have \(b-a=7\). Thus,
\(
7 m leq int_{-2}^5 f(x) mathrm{d} x leq 7 M
\)
11. The modulus property is given by
\(
left|int_a^b f(x) mathrm{d} xright| leq int_a^b|f(x)| mathrm{d} x .
\)
Proof:
From Negative of Absolute Value, we have for all \(a in[a ldots b]\) :
\(
-|f(t)| leq f(t) leq|f(t)|
\)
Thus from Relative Sizes of Definite Integrals:
\(
-int_a^b|f(t)| mathrm{d} t leq int_a^b f(t) mathrm{d} t leq int_a^b|f(t)| mathrm{d} t
\)
Hence the result.
12. Finally, we have a property for even and odd functions when integrating over the interval \([-a, a]\). For even functions \(f(-x)=f(x)\), we have
\(
int_{-a}^a f(x) mathrm{d} x=2 int_0^a f(x) mathrm{d} x .
\)
Example 8:
Evaluate \(int_{-pi / 2}^{pi / 2} cos ^3 x d x\)
Solution:
\(
begin{aligned}
&text { Let } f(x)=cos ^3 x \
&f(x)=(cos x)^3 \
&f(-x)=(cos (-x))^3 \
&f(-x)=(cos x)^3 \
&f(-x)=cos ^3 x \
&f(-x)=f(x)
end{aligned}
\)
The function \(f(x)\) is even.
\(
begin{aligned}
int_{-pi / 2}^{pi / 2} cos ^3 x d x &=2 int_0^{pi / 2} cos ^3 x d x \
&=2 int_0^{pi / 2} frac{(cos 3 x+3 cos x)}{4} \
&=(1 / 2)left[frac{sin 3 x}{3}+3 sin xright]_0^{pi / 2} \
&=(1 / 2)[(-1 / 3)+3)] \
&=(1 / 2)(8 / 3) \
&=4 / 3
end{aligned}
\)
For odd functions \(f(-x)=-f(x)\), we have
\(
int_{-a}^a f(x) mathrm{d} x=0
\)
Example 9:
Evaluate \(int_{-pi / 4}^{pi / 4} x^3 cos ^3 x d x\)
Solution:
\(
begin{aligned}
&int^{pi / 4} x^3 cos ^3 x d x \
&-pi / 4 \
&f(x)=x^3 cos ^3 x \
&f(x)=(x cos x)^3 \
&f(-x)=(-x cos (-x))^3 \
&f(-x)=-x cos ^3 x
end{aligned}
\)
The given function is odd.
\(
int_{-pi / 4}^{pi / 4} x^3 cos ^3 x d x=0
\)
13. \(int_a^b f(x) d x=int_a^b f(a+b-x) d x\)
Proof: Let \(u=a+b-x\)
\(
Rightarrow d u=-d x
\)
\(
int_a^b f(x) d x=int_a^b f(u) d u
\)
\(
begin{aligned}
&Rightarrow int_b^a f(a+b-x)(-d x) \
&Rightarrow-int_b^a f(a+b-x) d x \
&Rightarrow int_a^b f(a+b-x) d x
end{aligned}
\)
Hence Proved.
14. \(int_0^a f(x) d x=int_0^a f(a-x) d x\)
Proof:
\(I=int_0^a f(x) d x\)
now, put \(a-t=x; -d t=d x\)
also when,
\(
begin{aligned}
&x=0; t=a \
&x=a; t=0
end{aligned}
\)
\(
begin{array}{rlr}
I=int_a^0 f(a-t)(-d t)=int_0^a f(a-t) d t \
=int_0^a f(a-x) d x
end{array}
\)
Hence proved. The dummy variable does not affect the definite integral. So replacing \(t\) with \(x\) does not make any difference
15. \(int_0^{2 a} f(x) d x=int_0^a f(x) d x+int_0^a f(2 a-x) d x\)
Proof:
\(I=int_0^{2a} f(x) d x=int_0^a f(x) d x + int_a^{2 a} f(x) d x\)
now, put \(2a-x=t; -d t=d x\)
also when,
\(
begin{aligned}
&x=a; t=a \
&x=2a; t=0
end{aligned}
\)
Hence proved.
16. \(
int_0^{2 a} f(x) d x=left{begin{array}{l}
2 int_0^a f(x) d x, text { if } f(2 a-x)=f(x) \
0, text { if } f(2 a-x)=-f(x)
end{array}right.
\)
Proof:
Let’s use the following substitution
put \(2a-x=t; -d t=d x\)
also when,
\(
begin{aligned}
&x=a; t=a \
&x=2a; t=0
end{aligned}
\)
\(
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