Solveeit Logo

Question

Question: How do you integrate the function \(\ln 4x\) using integration by parts?...

How do you integrate the function ln4x\ln 4x using integration by parts?

Explanation

Solution

To simplify the integration, first assume 4x=t4x = t and convert the integration in the form of variable tt. Then apply integration by parts assuming lnt\ln t as first function and 1 as second function. The formula to use integration by parts is uvdx=uvdxdudx(vdx)dx\int {uvdx = u\int {vdx} } - \int {\dfrac{{du}}{{dx}}} \left( {\int {vdx} } \right)dx, here uu and vv are the functions of xx.

Complete step by step answer:
According to the question, we have to integrate the function ln4x\ln 4x using integration by parts.
Let this integration is denote by II then we have:
I=ln4xdx .....(1)\Rightarrow I = \int {\ln 4xdx} {\text{ }}.....{\text{(1)}}
Now if we substitute 4x=t4x = t then we have:
4dx=dt dx=dt4  \Rightarrow 4dx = dt \\\ \Rightarrow dx = \dfrac{{dt}}{4} \\\
Putting these values in the integration II, we have:
I=lntdt4 I=14lntdt  \Rightarrow I = \int {\ln t\dfrac{{dt}}{4}} \\\ \Rightarrow I = \dfrac{1}{4}\int {\ln tdt} \\\
The function lnt\ln t can be written as lnt×1\ln t \times 1. By doing this we will get:
I=14lnt(1)dt\Rightarrow I = \dfrac{1}{4}\int {\ln t\left( 1 \right)dt}
Now we can use integration by parts assuming lnt\ln t as first function and 1 as second function. The formula of integration by parts is shown below:
uvdx=uvdxdudx(vdx)dx\Rightarrow \int {uvdx = u\int {vdx} } - \int {\dfrac{{du}}{{dx}}} \left( {\int {vdx} } \right)dx, here uu and vv are the functions of xx.
Using this formula for the above integration, we have:
I=14[lntdtddtlnt(dt)dt]\Rightarrow I = \dfrac{1}{4}\left[ {\ln t\int {dt} - \int {\dfrac{d}{{dt}}\ln t\left( {\int {dt} } \right)dt} } \right]
We know the formulas ddxlnx=1x\dfrac{d}{{dx}}\ln x = \dfrac{1}{x} and dx=x\int {dx} = x. Using these formulas, we’ll get:
I=14[lnt(t)1t(t)dt+C]\Rightarrow I = \dfrac{1}{4}\left[ {\ln t\left( t \right) - \int {\dfrac{1}{t}\left( t \right)dt + C} } \right], here CC is the integration constant.
Simplifying it further, we’ll get:
I=14[tlntdt]+C4\Rightarrow I = \dfrac{1}{4}\left[ {t\ln t - \int {dt} } \right] + \dfrac{C}{4}
C4\dfrac{C}{4} is another constant. We will put it as KK.
I=14[tlntt]+K I=t4[lnt1]+K  \Rightarrow I = \dfrac{1}{4}\left[ {t\ln t - t} \right] + K \\\ \Rightarrow I = \dfrac{t}{4}\left[ {\ln t - 1} \right] + K \\\
Putting back the value t=4xt = 4x, we have:
I=4x4[ln4x1]+K I=x[ln4x1]+K  \Rightarrow I = \dfrac{{4x}}{4}\left[ {\ln 4x - 1} \right] + K \\\ \Rightarrow I = x\left[ {\ln 4x - 1} \right] + K \\\
Putting back the value of II from equation (1), we have:
ln4xdx=x[ln4x1]+K\Rightarrow \int {\ln 4xdx} = x\left[ {\ln 4x - 1} \right] + K
Thus this is the required integration.

Note: Whenever we have to integrate the multiple of two functions which cannot be integrated together while one of them can be integrated separately then we can apply integration by parts. The rule of integration by parts is given below:
uvdx=uvdxdudx(vdx)dx\Rightarrow \int {uvdx = u\int {vdx} } - \int {\dfrac{{du}}{{dx}}} \left( {\int {vdx} } \right)dx, here uu and vv are the functions of xx.
Here, we have assumed functions uu and vv cannot be integrated together. So we used integration by parts. However the function vv can be easily integrated which is why this method is helpful. For example in above case of integrating lnt(t)dt\int {\ln t\left( t \right)} dt, we took lnt\ln t as the first function and 1 as the second function.