Integration By Parts

The Organic Chemistry Tutor
25 Mar 202132:51

Summary

TLDRThis educational video script covers the technique of integration by parts to solve various integral problems. It explains the process step by step, starting with the integral of x times e^x and progressing to more complex examples such as the integral of x^2 ln(x) and combinations of exponential and trigonometric functions. The script also tackles integrals involving logarithmic functions and provides a method to solve definite integrals, exemplified by e^(3x)cos(4x). Each example builds on the previous, reinforcing the concept of integration by parts for students to master calculus integration.

Takeaways

  • πŸ“š Integration by parts is a fundamental technique for solving integrals of products of functions, expressed as ∫udv = uv - ∫vdu.
  • πŸ” Choosing 'u' and 'dv' wisely is crucial; typically, 'u' is chosen to simplify when differentiated, and 'dv' is chosen to be easily integrable.
  • πŸ“ˆ The integral of x * e^x is found by setting x as 'u' and e^x dx as 'dv', resulting in x * e^x - e^x + C.
  • πŸŒ€ For integrals involving trigonometric functions, such as x * sin(x), setting x as 'u' and sin(x) dx as 'dv' leads to -x * cos(x) + sin(x) + C.
  • πŸ“˜ When integrating a product of a polynomial and a logarithmic function, like x^2 * ln(x), it's often necessary to apply integration by parts multiple times.
  • ⚑ The integral of ln(x) is x * ln(x) - x + C, which is derived using integration by parts and recognizing the integral of 1 dx as x.
  • πŸ”— The integral of x^2 * sin(x) involves using integration by parts twice and results in a complex expression involving both sine and cosine functions.
  • 🌟 The integral of x^2 * e^x requires applying integration by parts twice, leading to a solution involving powers of e^x.
  • πŸ“‰ The integral of ln(x) squared involves rewriting the expression and applying integration by parts, resulting in x * ln(x) squared - 2x * ln(x) + 2x + C.
  • πŸ“Š The integral of ln(x) to the seventh power is simplified by recognizing it as 7 * ln(x), leading to 7 * (x * ln(x) - x) + C.
  • 🌌 The integral of e^x * sin(x) is solved by recognizing the pattern in the integral and using a clever manipulation to find the solution as (1/2) * e^x * (sin(x) - cos(x)) + C.

Q & A

  • What is the integral of x times e^x?

    -The integral of x times e^x is found using integration by parts, setting u=x and dv=e^x dx, which gives du=dx and v=e^x. The result is x * e^x - integral of e^x dx, which simplifies to x * e^x - e^x + C, where C is the constant of integration.

  • How do you integrate x times sine x dx?

    -For x times sine x, set u=x and dv=sine x dx, giving du=dx and v=-cosine x. Using integration by parts, the integral becomes -x * cosine x + integral of cosine x dx, which simplifies to -x * cosine x + sine x + C.

  • What is the antiderivative of x squared times ln x?

    -To find the antiderivative of x squared times ln x, set dv=x squared dx and u=ln x, giving v=x cubed / 3 and du=1/x dx. The integral by parts results in (1/3) * x cubed * ln x - (1/3) * integral of x squared dx, which simplifies to (1/3) * x cubed * ln x - (1/9) * x cubed + C.

  • How can you find the integral of the natural log of x using integration by parts?

    -For the natural log of x, set u=ln x and dv=dx, giving du=1/x dx and v=x. The integral by parts formula yields x * ln x - integral of x * (1/x) dx, which simplifies to x * ln x - x + C.

  • What is the indefinite integral of x squared times sine x dx?

    -For x squared times sine x, you need to use integration by parts twice. Initially, set u=x squared and dv=sine x dx, giving du=2x dx and v=-cosine x. The process involves further integration by parts on the resulting integral of 2x * cosine x dx, leading to a final answer involving x squared * cosine x, 2x * sine x, and 2 * cosine x, plus the constant C.

  • How do you integrate x squared times e^x dx?

    -For x squared times e^x, use integration by parts twice. Start by setting u=x squared and dv=e^x dx, giving du=2x dx and v=e^x. The process involves another round of integration by parts with u=2x and dv=e^x dx, leading to a final expression involving e^x terms and a constant C.

  • What is the integral of ln x squared dx?

    -To integrate ln x squared, set u=ln x squared and dv=dx, giving du=2 * ln x * (1/x) dx and v=x. The integral by parts results in x * ln x squared - 2 integral of ln x * (1/x) dx. Solving this requires recognizing the integral of ln x and simplifying to get the final answer involving x * ln x squared, -2x * ln x, and 2x, plus C.

  • How can you rewrite the integral of ln x to the seventh power dx?

    -The integral of ln x to the seventh power can be rewritten using the property of logs to move the exponent to the front, resulting in 7 * integral of ln x dx. Since the integral of ln x is x * ln x - x, the final answer is 7 * (x * ln x - x) + C.

  • What is the indefinite integral of e^x times sine x dx?

    -For e^x times sine x, set u=sine x and dv=e^x dx, giving du=cosine x dx and v=e^x. Using integration by parts, the process involves recognizing the similarity of the resulting terms to the original integral and solving for the integral, leading to a final answer involving e^x * (sine x - cosine x) / 2 plus C.

  • How do you find the antiderivative of ln x squared divided by x dx?

    -To find the antiderivative of ln x squared / x, rewrite it as ln x squared * 1/x dx and use integration by parts with u=ln x squared and dv=1/x dx, giving du=2 * ln x * (1/x) dx and v=ln x. The process involves recognizing the similarity of terms and solving for the integral, resulting in ln x cubed / 3 plus C.

  • What is the indefinite integral of e^(3x) times cosine 4x dx?

    -For e^(3x) times cosine 4x, set u=cosine 4x and dv=e^(3x) dx, giving du=-sine 4x * 4 dx and v=(1/3)e^(3x). Using integration by parts, the process involves moving constants to the front and recognizing the similarity of terms, leading to a final answer involving e^(3x) * (cosine 4x / 3 + 4/3 * sine 4x) plus C.

Outlines

00:00

πŸ“š Introduction to Integration by Parts

This paragraph introduces the concept of integration by parts, a technique used to find the integral of a product of two functions. It explains the formula for integration by parts, \( \int u \, dv = uv - \int v \, du \), and illustrates the process by setting up the functions 'u' and 'dv' for the integral of \( x \cdot e^x \). The explanation includes choosing 'u' and 'dv', finding 'du' and 'v', and applying the formula to arrive at the integral of \( x \cdot e^x \). It also briefly touches on the integral of \( x \cdot \sin(x) \) and \( x^2 \ln(x) \) as further examples.

05:01

πŸ” Detailed Walkthrough of Integration by Parts

The second paragraph delves deeper into the application of integration by parts with the integral of \( x \cdot \sin(x) \). It outlines the selection of 'u' and 'dv', calculates 'du' and 'v', and applies the formula to find the integral. The explanation continues with the integral of \( x^2 \ln(x) \), emphasizing the importance of choosing 'u' and 'dv' wisely to simplify the integration process. The paragraph concludes with the final answer for the integral of \( x^2 \ln(x) \) and introduces additional examples to practice the technique.

10:04

πŸ“˜ Advanced Integration by Parts Examples

This paragraph presents more complex examples of integration by parts, starting with the integral of \( x^2 e^x \). It discusses the strategy of choosing 'u' and 'dv' and the need for applying integration by parts multiple times due to the complexity of the function. The explanation proceeds with the integral of \( \ln(x) \) and \( x^2 \sin(x) \), demonstrating the process of repeatedly using integration by parts and simplifying the expressions to reach the final answers.

15:09

πŸ“™ Integration of Logarithmic and Exponential Functions

The fourth paragraph focuses on integrating functions involving logarithms and exponentials. It starts with the integral of \( \ln(x) \) using integration by parts and then moves on to the integral of \( x^2 e^x \), which requires a strategic approach to selecting 'u' and 'dv'. The explanation includes the step-by-step process of integrating these functions and concludes with the final expressions for each integral.

20:10

πŸ“’ Dealing with Higher Power Logarithms

This paragraph addresses the integration of higher power logarithmic functions, specifically \( \ln(x)^7 \). It explains how to rewrite the integral using logarithmic properties to simplify the process. The explanation demonstrates the integration of \( 7 \ln(x) \) and arrives at the final answer by applying the previously discussed anti-derivative of \( \ln(x) \).

25:12

πŸ“• Complex Exponential and Trigonometric Integrals

The sixth paragraph tackles the integration of complex functions involving exponentials and trigonometric functions, such as \( e^x \sin(x) \). It describes the process of using integration by parts and the need for careful selection of 'u' and 'dv'. The explanation includes the iterative application of integration by parts and the algebraic manipulation required to simplify the integral to its final form.

30:14

πŸ“” Integration of Products of Logarithms and Trigonometric Functions

The final paragraph discusses the integration of products of logarithmic and trigonometric functions, such as \( \ln(x)^2 / x \). It outlines the process of rewriting the integral and applying integration by parts, including the selection of 'u' and 'dv' and the calculation of 'du' and 'v'. The explanation concludes with the final answer for the integral and provides a method for solving similar problems.

πŸ““ Definite Integrals with Exponential and Trigonometric Functions

This paragraph explores the calculation of a definite integral involving \( e^{3x} \cos(4x) \). It suggests making the trigonometric function the 'u' in the integration by parts process and outlines the steps to find the integral. The explanation includes the manipulation of constants and the application of integration by parts multiple times to arrive at the final expression for the integral.

Mindmap

Keywords

πŸ’‘Indefinite Integral

An indefinite integral represents the family of all antiderivatives of a given function. It is the reverse process of differentiation and is denoted by the integral symbol ∫ without limits of integration. In the video, the indefinite integral is the main focus, with various functions being integrated to find their antiderivatives, such as x times e^x and x squared sine x.

πŸ’‘Integration by Parts

Integration by parts is a specialized method for integrating products of functions, based on the product rule for differentiation. It is expressed as ∫u dv = uv - ∫v du. The video script uses this technique multiple times to find the integrals of products like x times e^x and x squared times e^x, by choosing appropriate u and dv to simplify the integration process.

πŸ’‘Natural Logarithm (ln x)

The natural logarithm, denoted as ln x, is the logarithm of a number to the base e, where e is the Euler's number, an important mathematical constant. In the video, ln x is used in integrals such as the integral of ln x and ln x squared, which are solved using integration by parts and other integration techniques.

πŸ’‘Exponential Function (e^x)

An exponential function is a mathematical function of the form e^x, where e is the base of the natural logarithm. The video discusses the integration of exponential functions, especially when they are multiplied by other functions like x or sine x, and how to handle these using integration by parts.

πŸ’‘Trigonometric Functions

Trigonometric functions, such as sine and cosine, are periodic functions that relate angles to the ratios of two sides of a right triangle. The script covers the integration of products involving trigonometric functions, like x times sine x and e^x times sine x, demonstrating how to apply integration by parts to these cases.

πŸ’‘Derivative

A derivative represents the rate at which a function changes with respect to its variable. In the context of integration by parts, the derivative of a chosen function (u) is needed to find du. The script mentions finding derivatives of functions like x squared and ln x squared to apply the integration by parts formula.

πŸ’‘Antiderivatives

An antiderivative is a function that represents the reverse process of differentiation, essentially 'undoing' what the derivative does. The video's theme revolves around finding antiderivatives of various functions, such as x times e^x and ln x squared divided by x, using different integration techniques.

πŸ’‘Chain Rule

The chain rule is a method for finding the derivative of a composite function. In the script, the chain rule is implied when dealing with the derivative of ln x squared, which requires multiplying the derivative of the inner function (1/x) by the derivative of the outer function (2ln x).

πŸ’‘Constant of Integration (C)

The constant of integration, typically denoted as C, is added to the result of an indefinite integral to account for the infinite family of antiderivatives that differ by a constant. The script includes C in the final answers of integrals to indicate that the solution is an antiderivative plus an arbitrary constant.

πŸ’‘Power Rule

The power rule is a basic principle in calculus for finding the derivative of a function of the form x^n, where n is a constant. In the script, the power rule is applied when integrating functions like x squared, resulting in x to the power of (n+1) divided by (n+1).

πŸ’‘Product Rule

The product rule is a fundamental rule in calculus for differentiating the product of two functions. Although the video focuses on integration, the product rule is the basis for the integration by parts formula, which is derived from the product rule in reverse. The script uses integration by parts, which is essentially the product rule applied to integration.

Highlights

Introduction to finding the indefinite integral of x times e^x using integration by parts.

Setting u=x and dv=e^x dx for the integral of x times e^x.

Deriving the integral of e^x as e^x and applying integration by parts formula.

Solving the integral of x times sine x dx using integration by parts.

Choosing u=x and dv=sin(x)dx for the integral of x times sine x.

Finding the antiderivative of sine x as -cosine x and applying it to the integral.

Integrating x squared ln x using a strategic choice of u and dv.

Deciding on u=ln(x) and dv=x^2 dx for the integral of x squared ln x.

Using the derivative of ln(x) as 1/x to simplify the integral.

Deriving the integral of ln(x) as x ln(x) - x and applying integration by parts.

Integrating x squared sine x dx using a two-step integration by parts process.

Choosing u=x^2 and dv=sin(x)dx for the integral of x squared sine x, and applying integration by parts twice.

Solving the integral of x squared e^x dx using a two-step integration by parts approach.

Deciding on u=x^2 and dv=e^x dx for the integral of x squared e^x, and applying integration by parts twice.

Finding the indefinite integral of ln(x) squared dx using integration by parts.

Rewriting ln(x) squared as 2ln(x) and applying integration by parts.

Solving the integral of ln(x) to the power of seven using properties of logarithms.

Integrating e^x sin(x) dx using a recursive integration by parts strategy.

Rewriting the integral of ln(x) squared over x as a product of two functions.

Solving the definite integral of e^(3x)cos(4x) dx using integration by parts.

Applying integration by parts to the integral of e^(3x)sin(4x) dx and simplifying the result.

Transcripts

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so how can we find the indefinite

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integral of x

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times e raised to the x

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to do this

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we need to use something called

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integration by parts

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the integral of u

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dv

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is equal to u times v

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minus the integral of v

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d u

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so we need to determine u

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dv

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v

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and u and d u

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let me put it in a different order

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so which one should we set equal to u

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and which one

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should we set equal to dv

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it's best to set u

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equal to x

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because if we do so

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d u will simply be equal to one times dx

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and when dealing with constants

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they're a lot easier to integrate than

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variables

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so we're going to make dv equal to e to

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the x dx

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now v

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is the integral of dv

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the integral of e to the x is simply e

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to the x

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so now using the formula u times v

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that's going to be x

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times e raised to the x

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minus the integral of v

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d u

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v

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is e to the x d u is 1 dx

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and the integral of

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e to the x

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is e to the x plus some constant c

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so this is the final answer that's the

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integral

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of

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x raised to the or x times e raised to

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the x

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let's try another problem

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let's integrate x times sine x dx

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so what should we make u

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and

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dv equal to

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so just like before i'm going to make u

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equal to x

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so that d u is going to be 1

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dx

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now dv

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has to be what remains

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sine x

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dx

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now what is the integral of sine

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the derivative of what function will

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give us sign

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the integral of sine is negative cosine

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the derivative of negative cosine is

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positive sine

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so using the formula the integral of u

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dv

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is equal to u times v

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minus the integral of v

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d u

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so u is x

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v is negative cosine x

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and then minus v

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and d u is

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1 dx

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so far we have negative x

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cosine x

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and then these two negative signs will

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become positive so plus

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the integral of cosine x

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dx

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now the antiderivative of positive

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cosine

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is positive sine

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so the final answer

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is what you see here negative cosine i

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mean negative x cosine x

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plus sine x plus c

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now here's another problem to work on

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let's integrate x squared ln x

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so what should we make u

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and

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dv equal to in this problem

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if we make u equal to x squared

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and we make dv equal to ln x

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dx the integral of ln x

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will be quite difficult to do

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unless you know what it is so we're not

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going to do that

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so it's best to make

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dv

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x squared dx

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and u is going to be ln x because we

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know the derivative of l and x

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the derivative of l and x

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is 1 over x

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and the antiderivative of x squared

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the antiderivative of dv will give us v

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so the antiderivative of x squared dx

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is x cubed over 3.

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so let's use the formula now

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u times v that's going to be ln x times

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x cubed over three

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minus the integral of v

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times d u

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and

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d u is

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one over x

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it's supposed to be dx

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so this is equal to 1 3

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x cubed times ln x

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and then we could cancel an x and so we

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have minus one third the integral of x

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squared

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dx

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the integral of x squared is going to be

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x to the third over three

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and then plus some constant c

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so the final answer is one third

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x cubed ln x minus one over nine

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x to the third plus c

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and that concludes this problem

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so let's work on some more examples

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let's try this problem what is the

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anti-derivative

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of the natural log of x

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how can we use integration by parts to

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get this answer

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now we can't make u

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equal well we can't make a dv equal to l

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and x

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because we don't know the integral of l

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and x we're trying to figure that out so

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therefore we have to make u equal to

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ln x the derivative of that is one over

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x dx

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dv

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has to be

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just we can make dv dx if we want to

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or one dx

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and so v the integral of one dx is just

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x

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so now let's start with the formula

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and so it's going to be u times v

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u is ln x

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and v

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is x

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minus the integral of v

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and then d u

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is one over x

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dx

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so far we have x

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ln x

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x times one over x the x variables

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cancel

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so we have the integral of one

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dx now the integral of one dx is x

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so this is the final answer

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x ln x

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minus x plus c

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that is the integral

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of the natural log of x

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let's find the indefinite integral of x

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squared

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sine x

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dx

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so which part should be u

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and which part

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is going to be

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dv

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we need to make u equal to x squared

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and we need to differentiate it twice to

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bring it down to a constant so this is

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one of those problems where you have to

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use integration

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of you know integration by parts two

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times

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d u is going to be 2x dx

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dv

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is sine x dx

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so this is dv

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and this is going to be u

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the integral of sine

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is negative cosine

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so let's start with the formula

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so u times v that's x squared

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times negative cosine x

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minus

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the integral of v which is negative

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cosine x

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times d u

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that's

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2x dx

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so let's organize what we have negative

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x squared cosine x

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and then these two negative signs will

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become positive so positive the integral

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of

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2x cosine x

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we could take the 2 and move it to the

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front so it's just going to be x cosine

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x

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now we need to use the integration by

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parts formula

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on the integral of x cosine x

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we're going to make u equal to x

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and

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dv

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is going to be cosine x

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dx

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the integral of cosine is sine and the

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derivative of x is 1

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dx

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so using the formula

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it's going to be u times v

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which is

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x times sine x

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minus the integral

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of v d u

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so v is sine x

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d u is just dx

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and so the integral of sine

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is

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negative cosine

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and then plus c

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so now what we need to do is replace

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this part

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with what we have here

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so it's going to be plus we need to

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distribute 2 to everything in here

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so it's going to be 2x

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sine x

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plus

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this would be plus cosine x but times

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two so plus two cosine x

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and we don't need to multiply c by two

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because c is just

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some generic constant

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and

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this whole thing is equal to the

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original integral and so this is the

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answer

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negative x squared cosine x

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plus

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2x sine x

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plus 2 cosine x plus c

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now let's work on this problem

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let's say we have the integral of x

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squared

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e to the x dx

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go ahead and try that problem

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so let's begin by writing the formula

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the integral of u

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dv is equal to

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u times v minus the integral of v

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d u

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now what should we make u equal to

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and what should be

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dv

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i prefer making dv

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e c x dx

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because once we integrate it

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it's going to stay the same

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and i want x square to eventually become

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a constant so this is one of those

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problems where you need to do

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use the integration by parts formula

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twice

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so we're going to make u

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equal to x squared

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du is going to be 2x dx

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so using the formula it's going to be uv

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that's going to be

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x squared

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that's you v is e to the x

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minus the integral of v which is e to

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the x

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times d u that's 2x

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dx

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so now this becomes

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well before we uh do that let's use

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integration by parts one more time

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so i'm going to make u

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equal to 2x

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du is going to be the derivative of 2x

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which is 2 but times dx

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dv

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we're going to make that equal to

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e x dx

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just like we did before

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and the integral of that is simply e x

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so we're going to have

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x squared

play13:26

e x

play13:28

and then minus

play13:30

now let's use the formula again for this

play13:31

part so it's uv

play13:35

so 2x

play13:38

e to the x

play13:41

and then minus the integral

play13:43

of vdu

play13:45

so that's 2

play13:47

e to the x

play13:48

dx

play13:49

or multiplying those two

play13:54

now let's begin by distributing the

play13:56

negative signs

play14:00

so this is going to be negative 2x

play14:03

e to the x and then these two negatives

play14:05

will cancel

play14:07

giving us

play14:08

positive

play14:10

well let's take out the two so positive

play14:11

two integral

play14:13

e to the x dx

play14:15

so our final answer is going to be x

play14:17

squared

play14:18

e c x minus

play14:20

2 x e to the x

play14:22

anti derivative of e to the x is just e

play14:24

to the x and then plus c

play14:26

now if we want to we can factor out

play14:29

e to the x

play14:32

so we're going to have x squared minus

play14:34

2x

play14:35

plus 2 and then plus the constant c

play14:40

so this right here is our final answer

play14:42

that is the anti-derivative

play14:44

of

play14:45

x squared e to the x

play14:49

what about this problem

play14:51

what is the integral of

play14:53

ln x

play14:54

squared

play14:55

dx

play14:57

try that

play14:59

so for this problem what we need to do

play15:01

is we need to make u

play15:02

equal

play15:04

to ln x squared

play15:09

dv is going to be equal to the other

play15:11

part

play15:12

we're going to make dv

play15:14

equal to dx

play15:17

so v

play15:18

is going to be the integral of dx which

play15:20

is x

play15:21

d u i'm going to write that here i need

play15:23

more space

play15:24

we need to use the chain rule

play15:26

so first let's use the power rule by

play15:28

moving the 2 to the front

play15:30

so it's going to be 2 and then we'll

play15:32

keep everything on the inside the same 2

play15:34

times ln x

play15:35

and then we're going to subtract that by

play15:37

1

play15:38

and then take the derivative of the

play15:39

inside the derivative of l and x is one

play15:42

over x

play15:44

so using the formula this is going to be

play15:46

u times v

play15:49

so v is x u is

play15:52

ln x squared

play15:54

minus the integral of v d u

play15:57

v is x

play15:58

d u is

play16:00

2

play16:01

ln x

play16:03

times 1 of x and then

play16:05

let's not forget the dx part

play16:10

so we can cancel x and one of x

play16:14

so this becomes x

play16:18

ln x squared

play16:20

and then we could take out the two we

play16:21

can move it to the front so minus two

play16:24

integral

play16:25

ln x dx

play16:27

earlier in this video we determined that

play16:30

the integral of l and x is x ln x minus

play16:33

x

play16:38

so this is going to be -2

play16:40

and then we can replace this with

play16:43

x ln x minus x

play16:48

now let's go ahead and distribute the

play16:49

two so our final answer is going to be x

play16:53

times ln x squared

play16:55

minus 2x

play16:57

ln x

play16:58

and then negative 2 times negative x

play17:00

that's going to be positive

play17:03

2x and then plus c

play17:06

so this

play17:08

is

play17:09

the indefinite integral

play17:11

of ln x squared

play17:14

now what would you do if you were to see

play17:16

a problem like this

play17:18

ln x to the seventh power dx

play17:23

go ahead and try that

play17:26

well first you need to realize that we

play17:28

can rewrite this problem

play17:29

a property of logs allows us to move the

play17:32

exponent to the front

play17:34

so make sure you understand this this is

play17:35

not ln x

play17:37

to the seventh power like this

play17:40

if it was we can't move the seven

play17:42

the seven is only affecting the x

play17:44

variable as a result we can move the 7

play17:48

to the front

play17:49

so this becomes 7

play17:52

ln x

play17:54

so this is what we're integrating

play17:58

this is equivalent to 7

play18:00

integral

play18:02

ln x dx

play18:04

and we know the anti-derivative of l and

play18:05

x it's x

play18:07

ln x minus x

play18:11

so this is our final answer it's just 7

play18:14

x ln x

play18:16

minus 7 x plus c

play18:25

now let's try this one let's find the

play18:28

indefinite integral

play18:31

of e raised to the x sine x dx

play18:36

go ahead and work on that

play18:41

so for this problem i want to make

play18:44

u equal to sine x

play18:50

and then dv i'm going to set that equal

play18:52

to

play18:56

e to the x dx

play18:59

so v is simply going to be e to the x

play19:02

d u

play19:03

is the derivative of sine x which is

play19:06

cosine x

play19:08

so using the formula it's going to be

play19:10

uv

play19:12

that's going to be e

play19:14

sine x

play19:17

minus the integral of v d u

play19:19

so v is e to the x d u is cosine x dx

play19:25

so we need to use integration by parts

play19:27

one more time

play19:29

but this time we're going to make

play19:32

u equal to

play19:33

cosine x instead of sine

play19:38

and dv is going to be the same

play19:42

dv is going to be e to the x

play19:44

dx

play19:46

if v is the same

play19:48

d u is going to be the derivative of

play19:50

cosine which is negative

play19:52

sine

play19:54

and then times dx

play20:01

so now we're going to have

play20:04

e x

play20:05

sine x

play20:07

minus and then in brackets

play20:10

u v so that's going to be e x

play20:13

cosine x

play20:14

minus the integral of v to u

play20:17

so v is e to the x d u is

play20:20

negative

play20:22

sine x and then dx

play20:25

so let's go ahead and distribute the

play20:26

negative sign i'm going to rewrite the

play20:28

original integral

play20:30

so the integral of e x sine x

play20:34

that's going to be e to the x

play20:38

sine x

play20:41

these two negative signs

play20:43

will become positive

play20:45

and then we need to distribute this

play20:46

negative so it's negative e raised to

play20:49

the x cosine x

play20:51

and then we need to apply the negative

play20:52

to this

play20:53

which is going to be negative

play20:56

e to the x sine x

play20:58

now the key to solving this problem is

play21:00

to realize that this term is very

play21:03

similar to

play21:04

the original problem

play21:06

so what we want to do is we want to

play21:09

add this to both sides

play21:11

if we move it to the other side we're

play21:12

going to have 2

play21:14

e x sine x

play21:22

which is equal to this

play21:30

now we want to find the value of just

play21:32

one

play21:33

integral e to the x sine x

play21:36

so what we need to do is divide both

play21:38

sides

play21:39

by two

play21:42

so that's we can say that our final

play21:43

answer

play21:50

is one half

play21:54

we also factor out e to the x so it's

play21:57

one half e to the x

play21:59

and then times

play22:01

sine x

play22:03

minus cosine x

play22:05

plus c

play22:07

so that's the anti-derivative

play22:10

of

play22:11

e raised to the x times sine x

play22:16

now let's move on to our next example

play22:19

let's find the antiderivative of ln

play22:22

x squared

play22:24

divided by

play22:26

x dx

play22:28

so go ahead and try that

play22:31

now the first thing that i want to do is

play22:33

i'm going to rewrite this as

play22:37

ln x squared times 1 over x

play22:40

dx

play22:44

i want to multiply as a product of two

play22:45

functions

play22:47

now what i'm going to do is i'm going to

play22:48

make u

play22:50

equal to ln x

play22:52

squared

play22:55

du will be 2

play22:57

times ln x to the first power

play23:00

times 1 over x

play23:02

and then dx

play23:07

so since i made u ln x squared

play23:10

dv is going to be the other part

play23:12

dv is going to be 1 over x

play23:15

dx

play23:17

so anti-derivative of 1 over x is ln x

play23:22

now using the formula this is going to

play23:23

be u times v

play23:25

u is ln x

play23:27

squared

play23:28

v is just lnx

play23:31

minus the integral of vdu

play23:34

so v is ln x

play23:36

d u is 2

play23:39

ln x times 1 over x

play23:42

dx

play23:44

so let's put this all together so first

play23:46

i'm going to rewrite the original

play23:47

problem

play23:54

that's equal to ln x squared times ln x

play23:57

that's

play23:59

ln x raised to the third power

play24:04

in this 2 i'm going to move to the front

play24:07

here we have ln x times ln x

play24:11

that's ln x

play24:13

squared

play24:19

and it's multiplied by one over x which

play24:21

we can move that to the bottom

play24:25

and we need to realize that these two

play24:26

terms are similar

play24:28

so we need to add

play24:31

this to both sides or if we move it to

play24:34

the other side

play24:36

we'll basically add in 1

play24:38

plus 2 which will become 3. so on the

play24:40

left side we're going to have 3

play24:42

integral

play24:45

ln x

play24:47

squared

play24:49

over x dx

play24:52

and that's going to equal

play24:54

ln x

play24:56

to the third power

play24:58

so if we divide both sides by 3

play25:02

this 3 will disappear

play25:06

and we're going to have it underneath

play25:07

here

play25:09

and then plus our constant c

play25:12

so this

play25:13

is the answer

play25:14

to the original problem that's how we

play25:16

can find the integral of ln x squared

play25:18

over x

play25:20

now for the sake of practice go ahead

play25:22

and try this

play25:24

finding a definite integral of e to the

play25:25

3x cosine

play25:28

4x dx

play25:33

so whenever you have an e to the x times

play25:36

the sine or cosine

play25:37

it's good to make

play25:39

the cosine part

play25:41

equal to u

play25:42

that's what i'd like to do personally

play25:44

so in this one i'm going to make u equal

play25:46

to cosine

play25:48

4x

play25:49

du

play25:50

the derivative of cosine is going to be

play25:52

negative

play25:54

sine

play25:57

4x and then times the derivative of the

play26:00

angle the derivative of 4x is 4

play26:03

and then we're going to have times dx

play26:06

so dv in this problem

play26:10

is going to be e

play26:12

to the 3x to dx

play26:15

the antiderivative of e to the 3x it's e

play26:17

to the 3x over 3

play26:19

which

play26:20

we can write as one third e to the 3x

play26:24

so using the formula

play26:26

it's going to be uv

play26:28

so that's 1 3

play26:30

e to the 3x times cosine

play26:33

4x

play26:35

minus the integral

play26:37

of v d u

play26:40

so v

play26:41

is

play26:43

one third

play26:44

e to the three x

play26:46

d u

play26:48

that's

play26:49

negative

play26:50

four

play26:52

sine 4x

play26:55

dx

play27:01

so what we're going to do now is we're

play27:02

going to move the constants to the front

play27:07

the two negative signs

play27:10

will cancel they will become positive

play27:13

and we can move one third times four to

play27:15

the front

play27:16

so this is going to be plus

play27:19

four over three

play27:21

integral

play27:23

e to the three x

play27:25

sine four x dx

play27:29

now we need to use integration by parts

play27:30

one more time

play27:33

so dv will be the same we don't need to

play27:36

adjust this part of the formula

play27:39

but u

play27:40

is going to be sine 4x as opposed to

play27:44

cosine for x

play27:48

so du is going to change as well

play27:51

the derivative of sine is cosine

play27:54

4x

play27:56

and then times 4 times dx

play28:10

so using integration by parts we're

play28:12

going to have u times v

play28:14

so that's one-third

play28:19

e to the 3x times sine

play28:23

4x

play28:24

and then minus

play28:26

the integral of vdu

play28:28

so v is one third

play28:30

e to the three x

play28:32

and then d u that's times four

play28:35

cosine four x

play28:38

d x

play28:52

now let's go ahead and distribute four

play28:54

over three

play28:55

so multiply those together that's going

play28:57

to be

play28:58

4 over 9

play29:01

e to the 3x

play29:03

sine 4x

play29:06

and then this 2 will also be 4 over 9

play29:09

but it's going to be negative

play29:12

four over nine

play29:16

actually

play29:18

there's a four here so this is four

play29:21

thirds times four thirds

play29:23

so that's 16 over nine with a negative

play29:25

sign

play29:28

and then we're going to have the

play29:29

integral of e

play29:31

to the 3x

play29:33

cosine 4x

play29:35

dx

play29:48

now notice that these two are similar

play29:53

so we're going to add

play29:55

16 over 9 integral e to the 3x cosine

play29:58

4xdx to both sides

play30:00

so this is 1 but we can treat it as if

play30:02

it's

play30:04

9 over 9 just to get common denominators

play30:07

so 9 over 9 plus

play30:10

16 over 9

play30:11

that's going to be

play30:13

25

play30:14

over 9

play30:16

integral

play30:17

e to the 3x

play30:19

cosine 4x dx

play30:22

and then that's going to be 1 3

play30:25

e to the 3x cosine 4x

play30:29

and then plus

play30:31

4

play30:32

over 9

play30:33

e to the

play30:34

3x sine 4x

play30:43

now to get this to 1

play30:45

what we're going to do is we're going to

play30:46

multiply both sides by the reciprocal of

play30:50

25 over nine

play30:51

so that is by nine over twenty five

play30:55

so those two fractions will cancel

play30:58

on the left side we're just going to

play31:00

have

play31:01

e to the three x cosine four x

play31:03

dx

play31:07

and

play31:10

what i'm going to do

play31:12

i want to keep this in factored form

play31:15

so we have 9 over twenty five

play31:20

from one third and four over nine we can

play31:22

factor out one third

play31:25

and we can also factor out e to the

play31:27

three x

play31:32

so here we took out e to the three x

play31:34

we're left with just cosine four x

play31:38

here we took out e to the three x and we

play31:40

took out one third from four over nine

play31:42

so we're gonna have four thirds left

play31:44

over times sine 4x

play31:54

the last thing we could do is maybe

play31:56

reduce this

play31:58

so if we divide both numbers by 3 this

play32:01

becomes

play32:02

3

play32:03

over 25

play32:05

e to the 3x

play32:08

and then times

play32:10

cosine 4x plus 4 over 3

play32:15

sine 4x plus c

play32:20

so that's going to be the answer for

play32:22

this problem

play32:24

that's the indefinite integral of

play32:26

e to the 3x cosine 4x

play32:51

you

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