The definite integral we have studied so far can only apply to the continuous functions. Now we extend this definition to the function with finite number of discontinuity.
1st kind Improper Integral of the 1st kind applies to the case where the function has discontinuous points in the limit of integral.
If the integrand is continuous on and discontinuous at , then integrate from to . Then find the limit as approaches 0 from the right.
Note that the integral from to is the definite integral.
Improper Integral of the 1st kind [1] If is continuous on and discontinuous at . Then is continuous on the interval . Thus we can think of the following definite integral
1. 2.
First use u-substitution to make the integrand simple function. Then solve improper integral.
SOLUTION
1. Let
. Then and
.
,
.
SOLUTION 1. is continuous on , but discontinuous at . Let . Then , ,
Since the function is not continuous at , we may write . But it is better to take u-substitution first.
2. is continuous on , but not continuous at . Then we write
. .
Improper Integral of the 1st kind [3] is discontinuous at . Then divide the interval into subintervals . Now consider the improper imtegral on each subintervals. If all improper integrals exist, then we define the sum of improper integrals as improper integral of on .
SOLUTION is not continuous at . Then we write the integral as follows:
Improper Integral of the 2nd kind is continuous on . Then is continuous on , where . Then we define the infinite integral using the limit of .
This improper integral is used to find the convergence and divergence of other integral. For example,
is less than
and
converges. Thsu, converges.
SOLUTION
For ,
If is continuous on and exists, then we express this limit .
SOLUTION
Gamma Function Let . Then
is natural number
Gamma Function Gamma function was created to extend the factorial.
Proof
1.
Using integration by parts,
Maclaurin series expansion of is one of the most important series expansion. As we know the derivative of is . Then in the Maclaurin series expansion, every term is the derivative of the next term. Thus, . |
To find , we use the Maclaurin series expansion of .
2. By 1. for , we have the recurrence relation .
It is impossible to find . In other words, we can not express the indefinite integral of using elementary functions. |
In Example5.5, we have shown . Thus