The Art of the Shortcut
Mastering Integration by Parts
Welcome, fellow traveler on the path to JEE Advanced mastery. Today, we are tackling an integration problem that, at first glance, looks like a test of endurance.
We are asked to find the function g(x) defined by the integral ∫x3sinxdx and then evaluate a specific expression involving g(2π) and g′(2π).
Many students see x3sinx and immediately start writing out three rounds of integration by parts. While that is a valid path, it is also a path paved with potential for silly arithmetic errors. Today, we learn to be smarter, not just harder.
The Tabular Method
Your Secret Weapon
When you see a product of a polynomial and a trigonometric function, the Tabular Method (or DI Method) is your best friend. It is a structured, visual way to perform integration by parts repeatedly.
We set up three columns: one for the alternating sign, one for the function to differentiate (D), and one for the function to integrate (I).
We choose u=x3 for the D column because its derivative will eventually become zero, terminating the process. We choose dv=sinx for the I column because it is easy to integrate. We start with a positive sign, and then we alternate: (+),(−),(+),(−).
Following the steps:
1. Row 1: Sign (+), D term x3, I term sinx.
2. Row 2: Sign (−), D term 3x2, I term −cosx.
3. Row 3: Sign (+), D term 6x, I term −sinx.
4. Row 4: Sign (−), D term 6, I term cosx.
5. Row 5: Sign (+), D term 0, I term sinx.
By multiplying diagonally—Sign × D × I—we construct our function g(x):
g(x)=−x3cosx+3x2sinx+6xcosx−6sinx
The Fundamental Theorem of Calculus
A Moment of Clarity
Now, the problem asks for g′(2π). A novice would differentiate the entire expression we just found. But you? You know better.
By the Fundamental Theorem of Calculus, the derivative of the integral is simply the integrand itself. Therefore, g′(x)=x3sinx.
Evaluating this at x=2π is trivial:
g′(2π)=(2π)3sin(2π)=8π3
The Final Assembly
Now we evaluate g(2π). Look at our expression for g(x). Notice that cos(2π)=0.
This means the terms −x3cosx and 6xcosx vanish completely! We are left with:
g(2π)=3(2π)2sin(2π)−6sin(2π)=43π2−6
Finally, we substitute these into the expression 8(g(2π)+g′(2π)):
8[(43π2−6)+8π3]=6π2−48+π3
Comparing this to απ3+βπ2+γ, we find α=1, β=6, and γ=−48.
The final calculation α+β−γ=1+6−(−48)=55. You have conquered the problem with elegance and precision. Keep this mindset, and no integral will ever stand in your way.