Integration by parts may be daunting at first, especially it is comprised of different types of functions. Moreover, there are instances in evaluating integrals by integration by parts that there is a need to perform the process more than once. There are already available methods that don’t require this rigorous process anymore, hence evaluating integrals with such method can be further simplified.
The method that we will cover in this lesson is Tabular Integration by Parts, where we will tabulate the derivative of one function and the integral of the other repetitively. In order for us to make a good use of this method, let us have several examples that will show the different possible cases.
Case I: The u column reduces to zero “0’’
Example 1:
Evaluate the integral ∫x2sin2xdx
Solution:
In this method, we can still use the acronym LIATE in choosing the u and dv of the integrand. Since x2 is an algebraic function and sinx is a trigonometric function,
Let:u=x2dv=sin2xdx
In evaluating the integrals using the tabular method, create a column for u and another for dv. In the u column, differentiate the function, then write its derivative below it. Similarly, in the dv column, instead of differentiation, integrate the function, then continue the process.

When the u column reduces to zero “0”, stop the process. And to evaluate the integral, multiply each u with the dv diagonal lower from it bearing an alternating sign starting with positive (+).

Therefore,
∫x2sin2xdx=x2(−12cos2x)−2x(−14sin2x)+2(18cos2x)+C=−12x2cos2x+12xsin2x+14cos2x+CCase II: The product of the last row can be easily integrated
Example 2:
Evaluate the integral ∫x3lnxdx
Solution:
Since lnx is a logarithmic function and x3 is an algebraic function,
Let:u=lnxdv=x3dx

In instances where the u-column does not end up reducing to zero, but the product of the last row can already be easily integrated, the same solution as the first case can be used together with an additional step which is adding the integral of the product of the last row.
∫x3lnxdx=lnx⋅x44−∫x44⋅1xdx=x44lnx−14∫x3dx=x44lnx−14⋅x44+C=x44lnx−x416+CCase III: The original integral appears again
Example 3:
Evaluate the integral ∫e2xsin3xdx
Solution:

For this case, the original integral appears again, containing a different coefficient. This can be solved using the same solution as the second case.
∫e2xsin3xdx=12e2xsin3x−34e2xcos3x+94∫e2x(−sin3x)dx=12e2xsin3x−34e2xcos3x−94∫e2xsin3xdx∫e2xsin3xdx+94∫e2xsin3xdx=12e2xsin3x−34e2xcos3x+C134∫e2xsin3xdx=12e2xsin3x−34e2xcos3x+C∫e2xsin3xdx=413(12e2xsin3x−34e2xcos3x)+C=113(2e2xsin3x−3e2xcos3x)+CCase IV: Rows can be simplified
Example 4:
Evaluate the integral ∫ln2xdx
Evaluating integrals using the tabulation method sometimes may lead to a row that can be simplified. If this happens, we can rewrite the simplified functions to the next row, and a horizontal broken line can also be added to emphasize where the simplification occurs.

Hence,
∫ln2xdx=xln2x−2xlnx+2x+CCase V: Rows can be redistributed
Example 5:
Evaluate the integral ∫x3ex2dx
In cases where simplification may not be enough, we can also redistribute variables to another column in a row. A horizontal broken line can also be added to emphasize where the redistribution occurs.

Hence,
∫x3ex2dx=12x2e2x−2⋅14ex2+C=12x2e2x−12ex2+C