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Evaluate the following integrals. $$\int_{1}^{2 e} \frac{3^{\ln x}}{x} d x$$

Short Answer

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Question: Evaluate the definite integral of the given function:$$\int_{1}^{2 e} \frac{3^{\ln x}}{x} d x$$ Answer: The definite integral of the given function is $$\int_{1}^{2 e} \frac{3^{\ln x}}{x} d x = \frac{(2e)^{\ln 3} - 1}{\ln 3}$$

Step by step solution

01

Recall the properties of exponents and logarithms

Recall that for any positive number \(a\), we have $$a^{\ln x}=x^{\ln a}$$ This property allows us to rewrite the given integrand.
02

Rewrite the integrand using the property

Using the property from step 1, we can rewrite the integrand as: $$\frac{3^{\ln x}}{x} = \frac{x^{\ln 3}}{x}$$ Now, we simplify the expression: $$\frac{x^{\ln 3}}{x} = x^{\ln 3 - 1}$$
03

Evaluate the antiderivative

To evaluate the given integral, we need to find the antiderivative of the simplified integrand. Since we have a power function, we can use the power rule: $$\int x^{n} d x = \frac{x^{n+1}}{n+1} + C$$ Applying this rule to our integrand, we have: $$\int x^{\ln 3 - 1} d x = \frac{x^{\ln 3}}{\ln 3} + C$$
04

Evaluate the definite integral

Now that we have calculated the antiderivative, we can evaluate the definite integral by plugging in the bounds of integration: $$\int_{1}^{2e} x^{\ln 3 - 1} d x = \frac{x^{\ln 3}}{\ln 3} \Big|_{1}^{2 e}$$ Evaluate the antiderivative at the upper and lower bounds: $$\frac{(2e)^{\ln 3}}{\ln 3} - \frac{1^{\ln 3}}{\ln 3}$$
05

Simplify the result

Simplify the expression to obtain the final result: $$\frac{(2e)^{\ln 3}}{\ln 3} - \frac{1^{\ln 3}}{\ln 3} = \frac{(2e)^{\ln 3} - 1}{\ln 3}$$ So, $$\int_{1}^{2 e} \frac{3^{\ln x}}{x} d x = \frac{(2e)^{\ln 3} - 1}{\ln 3}$$

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Key Concepts

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

Definite Integrals
Definite integrals are a fundamental concept in calculus, representing the area under a curve between two specified points, called bounds. When you calculate a definite integral, you are essentially finding the signed area between a function's graph and the x-axis from one point to another. In the context of the exercise, the definite integral is given from the bounds 1 to 2e. This means we are interested in the accumulated area of the function \( \frac{3^{\ln x}}{x} \) from \( x = 1 \) to \( x = 2e \).
  • The process involves finding the antiderivative (a function whose derivative is the original function) and then evaluating this at the two bounds, subtracting the value at the lower bound from the value at the upper bound.
  • The result is often a number or, as in this exercise, an expression that simplifies to a finite value.
Understanding definite integrals is crucial because they can calculate quantities, like area, volume, and other values that express accumulation over an interval.
Antiderivatives
Antiderivatives are the inverse operation of derivatives. If a function \( F(x) \) is an antiderivative of \( f(x) \), then the derivative of \( F(x) \) is \( f(x) \). This relationship is symbolized by \( F'(x) = f(x) \). Antiderivatives are essential in solving integrals, especially definite integrals. In this exercise, we needed the antiderivative of the simplified function \( x^{\ln 3 - 1} \).
  • The power rule for antiderivatives states that for any function of the form \( x^n \), the antiderivative is \( \frac{x^{n+1}}{n+1} + C \), where \( C \) is the constant of integration.
  • Applying the power rule enabled us to find \( \int x^{\ln 3 - 1} \, dx = \frac{x^{\ln 3}}{\ln 3} + C \).
Antiderivatives are the pathway to calculating definite integrals. Once you have the antiderivative, evaluate it using the limits of integration to find the total area or accumulated value.
Properties of Logarithms and Exponents
Logarithms and exponents have several properties that simplify expressions and solve integrals. One vital property is that \( a^{\ln b} = b^{\ln a} \). This enables transformations that make integration more feasible. For our exercise, this property allowed the conversion of \( 3^{\ln x} \) into \( x^{\ln 3} \). Here's why these properties are essential:
  • They facilitate the rewriting of complex expressions into simpler forms, suitable for integration or differentiation.
  • They offer computational shortcuts that can save significant time and effort when evaluating complex integrals.
Using these properties not only simplifies functions but also clarifies their behavior, helping us solve them more efficiently. Understanding how logarithms and exponents interrelate is key to mastering integral calculus.

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Most popular questions from this chapter

When an object falling from rest encounters air resistance proportional to the square of its velocity, the distance it falls (in meters) after \(t\) seconds is given by \(d(t)=\frac{m}{k} \ln [\cosh (\sqrt{\frac{k g}{m}} t)],\) where \(m\) is the mass of the object in kilograms, \(g=9.8 \mathrm{m} / \mathrm{s}^{2}\) is the acceleration due to gravity, and \(k\) is a physical constant. a. A BASE jumper \((m=75 \mathrm{kg})\) leaps from a tall cliff and performs a ten-second delay (she free-falls for 10 s and then opens her chute). How far does she fall in \(10 \mathrm{s} ?\) Assume \(k=0.2\) b. How long does it take for her to fall the first \(100 \mathrm{m} ?\) The second 100 \(\mathrm{m} ?\) What is her average velocity over each of these intervals?

Evaluate the following integrals. \(\int \frac{\cosh z}{\sinh ^{2} z} d z\)

a. Confirm that the linear approximation to \(f(x)=\tanh x\) at \(a=0\) is \(L(x)=x\) b. Recall that the velocity of a surface wave on the ocean is \(v=\sqrt{\frac{g \lambda}{2 \pi} \tanh \left(\frac{2 \pi d}{\lambda}\right)} .\) In fluid dynamics, shallow water refers to water where the depth-to-wavelength ratio \(d / \lambda<0.05 .\) Use your answer to part (a) to explain why the shallow water velocity equation is \(v=\sqrt{g d}\) c. Use the shallow-water velocity equation to explain why waves tend to slow down as they approach the shore.

Alternative proof of product property Assume that \(y>0\) is fixed and that \(x>0 .\) Show that \(\frac{d}{d x}(\ln x y)=\frac{d}{d x}(\ln x) .\) Recall that if two functions have the same derivative, they differ by an additive constant. Set \(x=1\) to evaluate the constant and prove that \(\ln x y=\ln x+\ln y.\)

A spring has a restoring force given by \(F(x)=25 x .\) Let \(W(x)\) be the work required to stretch the spring from its equilibrium position \((x=0)\) to a variable distance \(x\) Graph the work function. Compare the work required to stretch the spring \(x\) units from equilibrium to the work required to compress the spring \(x\) units from equilibrium.

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