/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 32 Evaluate the following integrals... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

Evaluate the following integrals using integration by parts. $$\int_{0}^{1} x^{2} 2^{x} d x$$

Short Answer

Expert verified
Question: Evaluate the integral: $\int_{0}^{1} x^{2} 2^{x} d x$ Answer: The integral evaluates to $\frac{1}{\ln(2)} - \frac{2}{\ln(2)^3}$.

Step by step solution

01

Choose u and dv

Set u equal to \(x^2\) and dv equal to \(2^x dx\).
02

Find du and v

Differentiate u to find du: \(du = 2x \, dx\). Integrate dv to find v: \(v = \int 2^{x} \, dx = \frac{1}{\ln(2)}2^x\).
03

Apply integration by parts

Using the formula \(\int u \, dv = uv - \int v \, du\), we have: $$\int_{0}^{1} x^{2} 2^{x} d x = \left[x^2 \frac{1}{\ln(2)} 2^x\right]_0^1 - \int_{0}^{1} \frac{1}{\ln(2)}2^x \cdot 2x \, dx$$
04

Simplify the expression

Now, we need to simplify the integral and evaluate it: $$\left[x^2 \frac{1}{\ln(2)} 2^{x}\right]_0^1 - \frac{2}{\ln(2)} \int_{0}^{1} x 2^{x} dx$$
05

Apply integration by parts again

Now, for the remaining integral, let \(u = x\) and \(dv = 2^x dx\), and find \(du\) and \(v\): \(du = dx\) and \(v = \frac{1}{\ln(2)}2^x\). Apply the integration by parts formula: $$\int_{0}^{1} x 2^{x} d x = \left[ x \frac{1}{\ln(2)} 2^x \right]_0^1 - \int_{0}^{1} \frac{1}{\ln(2)} 2^x dx$$
06

Simplify and evaluate

Now, evaluate the definite integrals and simplify: $$\left[ x \frac{1}{\ln(2)} 2^x \right]_0^1 - \left[ \frac{1}{\ln{2}^2} 2^x\right]_0^1 = \frac{1}{\ln(2)} - \frac{1}{\ln{2}^2}(2 - 1)$$
07

Substituting back

Now, substitute this result back into the first integral: $$\left[ x^2 \frac{1}{\ln(2)} 2^x\right]_0^1 - \frac{2}{\ln(2)}\left(\frac{1}{\ln(2)} - \frac{1}{\ln{2}^2}\right)$$
08

Final evaluation

Evaluating the expression gives the result: $$\frac{1}{\ln(2)} - \frac{2}{\ln(2)^2}\left(\frac{1}{\ln(2)} - \frac{1}{\ln{2}^2}\right) = \frac{1}{\ln(2)} - \frac{2}{\ln(2)^3}$$ Thus, $$\int_{0}^{1} x^{2} 2^{x} d x = \frac{1}{\ln(2)} - \frac{2}{\ln(2)^3}$$

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with 91Ó°ÊÓ!

Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Definite Integrals
Definite integrals represent the net area under a curve over a given interval. In the context of our example, where we are solving \[\int_{0}^{1} x^{2} 2^{x} d x\], the definite integral is evaluated from the lower limit of 0 to the upper limit of 1. This specific integral is challenging because it combines polynomial and exponential functions, requiring advanced techniques like integration by parts to solve. The process involves subtracting the area below the x-axis from the total area when the graph dips below.

To evaluate definite integrals with accuracy, it is essential to understand the limits of integration and the function behavior within these limits. This includes knowing when and how to apply properties of definite integrals, such as linearity, additivity, and their relationship with antiderivatives.
Exponential Functions
Exponential functions are vital in calculus due to their unique properties; they remain unchanged when differentiated or integrated. In our exercise, the function \(2^{x}\) represents an exponential function with base 2. Exponential functions grow or decay at a rate proportional to their current value, which is why they often model real-world phenomena like population growth or radioactive decay.

When integrating exponential functions, especially during integration by parts, it is crucial to identify the right part of the function to set as \(dv\) in the integration by parts formula. In our step-by-step solution, \(2^{x} dx\) is selected as \(dv\) because its integral is known and manageable, leading to a simpler integral for further steps.
Antiderivatives
The antiderivative, also known as an indefinite integral, is the inverse process of differentiation. When finding the antiderivative of a function, you are essentially determining a function whose derivative is the original function. It's used extensively in the process of integration by parts, which is essentially the integration application of the product rule of differentiation.

In our exercise, finding the antiderivative of \(2^{x}\) required recognizing that it equated to \(\frac{1}{\ln(2)}2^x\), which then allowed for the integration by parts process to proceed. It's important to correctly compute antiderivatives to avoid errors in solving definite integrals, and these computations provide the foundation for determining areas under curves and solving differential equations.

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

Estimating error Refer to Theorem 8.1 in the following exercises. Let \(f(x)=\sqrt{\sin x}\) a. Find a Simpson's Rule approximation to \(\int_{1}^{2} \sqrt{\sin x} d x\) using \(n=20\) subintervals. b. Find an upper bound on the absolute error in the estimate found in part (a) using Theorem 8.1. (Hint: Use the fact that \(\left.\left|f^{(4)}(x)\right| \leq 1 \text { on }[1,2] .\right)\)

Normal distribution of movie lengths A study revealed that the lengths of U.S. movies are normally distributed with a mean of 110 minutes and a standard deviation of 22 minutes. This means that the fraction of movies with lengths between \(a\) and \(b\) minutes (with \(a

Evaluate \(\int_{0}^{\pi / 4} \ln (1+\tan x) d x\) using the following steps. a. If \(f\) is integrable on \([0, b],\) use substitution to show that $$\int_{0}^{b} f(x) d x=\int_{0}^{b / 2}(f(x)+f(b-x)) d x$$ b. Use part (a) and the identity tan \((\alpha+\beta)=\frac{\tan \alpha+\tan \beta}{1-\tan \alpha \tan \beta}\) to evaluate \(\int_{0}^{\pi / 4} \ln (1+\tan x) d x\) (Source: The College Mathematics Journal, \(33,4,\) Sep 2004 )

The work required to launch an object from the surface of Earth to outer space is given by \(W=\int_{R}^{\infty} F(x) d x,\) where \(R=6370 \mathrm{km}\) is the approximate radius of Earth, \(F(x)=\frac{G M m}{x^{2}}\) is the gravitational force between Earth and the object, \(G\) is the gravitational constant, \(M\) is the mass of Earth, \(m\) is the mass of the object, and \(G M=4 \times 10^{14} \mathrm{m}^{3} / \mathrm{s}^{2}\) a. Find the work required to launch an object in terms of \(m\). b. What escape velocity \(v_{e}\) is required to give the object a kinetic energy \(\frac{1}{2} m v_{e}^{2}\) equal to \(W ?\) c. The French scientist Laplace anticipated the existence of black holes in the 18 th century with the following argument: If a body has an escape velocity that equals or exceeds the speed of light, \(c=300,000 \mathrm{km} / \mathrm{s},\) then light cannot escape the body and it cannot be seen. Show that such a body has a radius \(R \leq 2 G M / c^{2} .\) For Earth to be a black hole, what would its radius need to be?

Comparing the Midpoint and Trapezoid Rules Compare the errors in the Midpoint and Trapezoid Rules with \(n=4,8,16,\) and 32 subintervals when they are applied to the following integrals (with their exact values given). $$\int_{0}^{1}\left(8 x^{7}-7 x^{8}\right) d x=\frac{2}{9}$$

See all solutions

Recommended explanations on Math Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.