Chapter 5: Problem 25
As needed, use a computer to plot graphs and to check values of integrals. By changing to polar coordinates, evaluate $$\int_{0}^{\infty} \int_{0}^{\infty} e^{-\sqrt{x^{2}+y^{2}}} d x d y.$$
Short Answer
Expert verified
The value of the integral is \(\textstyle 2\pi\).
Step by step solution
01
Understand the Integral
Given the double integral \(\textstyle \int_{0}^{\infty} \int_{0}^{\infty} e^{-\sqrt{x^{2}+y^{2}}} d x d y\), the goal is to evaluate it by changing to polar coordinates.
02
Set Up the Polar Coordinates Transformation
In polar coordinates, \((x, y) = (r \cos \theta, r \sin \theta)\) and the Jacobian of the transformation is \(|J| = r\). Moreover, \(\textstyle x^2 + y^2 = r^2\). Hence, the integral becomes \(\textstyle \int_{0}^{\infty} \int_{0}^{2\pi} e^{-r} r d\theta d r\).
03
Evaluate the \( \theta \) Integral
Integrate with respect to \theta, keeping \r as a constant: \(\textstyle \int_{0}^{2\pi} e^{-r} r d\theta = r e^{-r} \int_{0}^{2\pi} d\theta = r e^{-r} \cdot 2\pi\).
04
Simplify the Integral
The integral now simplifies to \(\textstyle 2\pi \int_{0}^{\infty} r e^{-r} d r\).
05
Evaluate the Remaining Integral
Consider the integral \(\textstyle \int_{0}^{\infty} r e^{-r} d r\). Use integration by parts where \(\textstyle u = r\) and \(\textstyle dv = e^{-r} dr\), hence \(\textstyle du = dr\) and \(\textstyle v = -e^{-r} \). Applying integration by parts, we get \(\textstyle \int_{0}^{\infty} r e^{-r} d r = \left[ -r e^{-r} \right]_{0}^{\infty} + \int_{0}^{\infty} e^{-r} d r\).
06
Solve the Evaluated Expression
The boundary term \(\textstyle \left[ -r e^{-r} \right]_{0}^{\infty} = 0\) since \(\textstyle \lim_{r \to \infty} -r e^{-r} = 0\) and \(\textstyle -0 \cdot e^{-0} = 0\). Thus, we have \(\textstyle \int_{0}^{\infty} r e^{-r} d r = \int_{0}^{\infty} e^{-r} d r = \left[ -e^{-r} \right]_{0}^{\infty} = 1\).
07
Combine All Results
Combining the results, \(\textstyle 2\pi \int_{0}^{\infty} r e^{-r} d r = 2\pi \cdot 1 = 2\pi\).
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Double Integral
A double integral is a way to integrate over a two-dimensional area. It's basically adding up little pieces of area (much like how a single integral adds up line segments). When dealing with functions of two variables, a double integral gives you a way to find the volume under a surface defined by those variables.
For example, the double integral \textstyle \int_{0}^{\infty} \int_{0}^{\infty} e^{-\sqrt{x^{2}+y^{2}}} \, dx \, dy}\, tells us to sum up all the tiny areas under the surface described by \textstyle e^{-\sqrt{x^{2}+y^{2}}}\, across all positive \( x \) and \( y \) values.
We typically write double integrals like this:
For example, the double integral \textstyle \int_{0}^{\infty} \int_{0}^{\infty} e^{-\sqrt{x^{2}+y^{2}}} \, dx \, dy}\, tells us to sum up all the tiny areas under the surface described by \textstyle e^{-\sqrt{x^{2}+y^{2}}}\, across all positive \( x \) and \( y \) values.
We typically write double integrals like this:
- Inner integral (\(dy\)) integrates respect to \(y\), treating \(x\) as a constant.
- Outer integral (\(dx\)) integrates the result of the inner integral, this time with respect to \(x\).
Polar Coordinates
Polar coordinates, represented as \((r, \theta)\), describe points in the plane using a distance from the origin (\(r\)) and an angle from the positive x-axis (\(\theta\)).
For conversion:
Using these transformations, the region of integration becomes simpler, and the integral \textstyle \int_{0}^{\infty} \int_{0}^{\infty} e^{-\sqrt{x^{2}+y^{2}}} \, dx \, dy\ changes to \textstyle \int_{0}^{\infty} \int_{0}^{2\pi} e^{-r} \, r \, d\theta \, dr}\.
Notice that the limits simplify as well: \(r\) ranges from \(0\) to \(\infty\), and \(\theta\) ranges from \(0\) to \(2\pi\). This greatly simplifies the integral.
For conversion:
- \(x = r \, \cos \theta\)
- \(y = r \, \sin \theta\)
- \(dx \, dy = r \, dr \, d\theta\)
Using these transformations, the region of integration becomes simpler, and the integral \textstyle \int_{0}^{\infty} \int_{0}^{\infty} e^{-\sqrt{x^{2}+y^{2}}} \, dx \, dy\ changes to \textstyle \int_{0}^{\infty} \int_{0}^{2\pi} e^{-r} \, r \, d\theta \, dr}\.
Notice that the limits simplify as well: \(r\) ranges from \(0\) to \(\infty\), and \(\theta\) ranges from \(0\) to \(2\pi\). This greatly simplifies the integral.
Integration by Parts
Integration by parts is a technique used to solve integrals where the standard methods aren't straightforward. It is based on the product rule for differentiation and is given by:
(uv - \int v \, du).
In the problem's context, to integrate \textstyle \int_{0}^{\infty} r e^{-r} \, dr\}, we set it up as:
\textstyle \int_{0}^{\infty} r e^{-r} \, dr = [ -r e^{-r} ]_{0}^{\infty} + \int_{0}^{\infty} e^{-r} \, dr\. Both boundary terms resolve to 0 due to limits. Simplifying further, we integrate \(e^{-r}\) from 0 to \(\infty\), resulting in 1.
This allows us to evaluate our original integral fully.
(uv - \int v \, du).
In the problem's context, to integrate \textstyle \int_{0}^{\infty} r e^{-r} \, dr\}, we set it up as:
- \(u = r\)
- \(dv = e^{-r} \, dr\)
- \(du = dr\)
- \(v = -e^{-r}\)
\textstyle \int_{0}^{\infty} r e^{-r} \, dr = [ -r e^{-r} ]_{0}^{\infty} + \int_{0}^{\infty} e^{-r} \, dr\. Both boundary terms resolve to 0 due to limits. Simplifying further, we integrate \(e^{-r}\) from 0 to \(\infty\), resulting in 1.
This allows us to evaluate our original integral fully.