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By expressing both the integrand and the surface element in spherical polar coordinates, show that the surface integral $$ \int \frac{x^{2}}{x^{2}+y^{2}} d S $$ over the surface \(x^{2}+y^{2}=z^{2}, 0 \leq z \leq 1\), has the value \(\pi / \sqrt{2}\).

Short Answer

Expert verified
The value of the surface integral is \( \frac{\pi}{\sqrt{2}} \).

Step by step solution

01

- Convert Cartesian Coordinates to Spherical Coordinates

Using spherical coordinates, express the Cartesian coordinates as follows: \(x = \rho \, \sin \theta \, \cos \phi\), \(y = \rho \, \sin \theta \, \sin \phi\), and \(z = \rho \, \cos \theta\).
02

- Identify the Surface Equation

The surface is given by \(x^2 + y^2 = z^2\). In spherical coordinates, this becomes \(\rho^2 \, \sin^2 \theta = \rho^2 \, \cos^2 \theta\). Thus, \( \tan^2 \theta = 1 \) or \( \theta = \frac{\pi}{4} \).
03

- Set Up the Integral in Spherical Coordinates

Given \( \theta = \frac{\pi}{4} \) on the surface, express the integrand and surface element accordingly: Integrand: \( \frac{x^2}{x^2 + y^2} = \frac{\rho^2 \, \sin^2 \theta \, \cos^2 \phi}{\rho^2 \, \sin^2 \theta} = \cos^2 \phi \). Surface element: \( dS = \rho^2 \, \sin \theta \, d\phi \, d\rho\).
04

- Evaluate the Surface Integral

Express the integral in terms of \( \phi \) and \( \rho \): \[ \int_0^{2\pi} \int_0^1 \cos^2 \phi \, \rho^2 \, \sin \ \frac{\pi}{4} \, d\rho \, d\phi \]. Since \( \sin \ \frac{\pi}{4} = \frac{\sqrt{2}}{2} \): \[ \int_0^{2\pi} \int_0^1 \cos^2 \phi \, \frac{\rho^2 \sqrt{2}}{2} \, d\rho \, d\phi \].
05

- Simplify and Integrate

Simplify the integral and integrate separately over \( \rho \) and \( \phi \): \[ \frac{\sqrt{2}}{2} \int_0^{2\pi} \cos^2 \phi \, d\phi \int_0^1 \rho^2 \, d\rho \]. Integrate \( \rho^2 \): \[ \int_0^1 \rho^2 \, d\rho = \left[ \frac{\rho^3}{3} \right]_0^1 = \frac{1}{3} \]. Integrate \( \cos^2 \phi \): \( \int_0^{2\pi} \cos^2 \phi \, d\phi = \pi \). The final value is: \( \frac{\sqrt{2}}{2} \times \frac{\pi}{3} = \frac{\pi \sqrt{2}}{6} \).

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Key Concepts

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

spherical coordinates
Spherical coordinates are an alternative to Cartesian coordinates for describing points in three-dimensional space. They are particularly useful when dealing with problems that have symmetry about a point, such as spheres and cones. In spherical coordinates, a point is represented by three values:
  • \rho (rho) - the radial distance from the origin to the point
  • \theta (theta) - the polar angle, measured from the positive z-axis
  • \theta (phi) - the azimuthal angle, measured from the positive x-axis in the xy-plane

The coordinates are converted by: \(x = \rho \, \sin \theta \, \cos \phi\), \(y = \rho \, \sin \theta \, \sin \phi\), and \(z = \rho \, \cos \theta\). These transformations help simplify the equations and integrals when dealing with three-dimensional objects.
surface integrals
Surface integrals extend the concept of integrals to functions over a surface in three-dimensional space. They are essential in physics and engineering to calculate quantities like flux and surface area. To evaluate a surface integral, you often need to:
  • Describe the surface parametrically
  • Determine the differential surface area element, \(dS\)
  • Express the integrand in the chosen coordinates

For example, given a surface defined by \(x^2 + y^2 = z^2\), the surface integral of a function \(f(x, y, z)\) can be calculated by converting it into spherical coordinates and then integrating over the surface.
coordinate transformations
Coordinate transformations change the system of coordinates used to describe a point or a function. This can simplify equations and integrals in many cases. The most common transformations are:
  • Cartesian to spherical coordinates
  • Cartesian to cylindrical coordinates

For spherical coordinates, the transformations are:
  • \( x = \rho \, \sin \theta \, \cos \phi \)
  • \( y = \rho \, \sin \theta \, \sin \phi \)
  • \( z = \rho \, \cos \theta \)

These transformations are very useful in simplifying the evaluation of integrals over curved surfaces, such as spheres and cones. Coordinate transformations are key in multivariable calculus because they adapt the integration process to better match the problem's geometry and symmetry properties.
multivariable calculus
Multivariable calculus extends the principles of calculus to functions of multiple variables. It involves:
  • Partial derivatives
  • Multiple integrals
  • Vector calculus

Surface integrals are a critical component of multivariable calculus, allowing for the integration of functions over surfaces in three dimensions. To work effectively with these integrals, one often uses coordinate transformations to switch between Cartesian, cylindrical, and spherical coordinates.
For example, in the exercise, the integration over the surface \( x^2 + y^2 = z^2 \) was simplified using spherical coordinates. Understanding how to switch coordinate systems and work with differentials in these systems is essential for solving complex integrals in multivariable calculus.

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Most popular questions from this chapter

Sketch the domain of integration for the integral $$ I=\int_{0}^{1} \int_{x-y}^{1 / y} \frac{y^{3}}{x} \exp \left[y^{2}\left(x^{2}+x^{-2}\right)\right] d x d y $$ and characterise its boundaries in terms of new variables \(u=x y\) and \(v=y / x\). Show that the Jacobian for the change from \((x, y)\) to \((u, v)\) is equal to \((2 v)^{-1}\), and hence evaluate \(I\).

A planar figure is formed from uniform wire and consists of two semicircular arcs, each with its own closing diameter, joined so as to form a letter ' \(B\) '. The figure is freely suspended from its top left-hand corner. Show that the straight edge of the figure makes an angle \(\theta\) with the vertical given by \(\tan \theta=(2+\pi)^{-1}\).

The shape of an axially symmetric hard-boiled egg, of uniform density \(\rho_{0}\), is given in spherical polar coordinates by \(r=a(2-\cos \theta)\), where \(\theta\) is measured from the axis of symmetry. (a) Prove that the mass \(M\) of the egg is \(M=\frac{40}{3} \pi \rho_{0} a^{3}\). (b) Prove that the egg's moment of inertia about its axis of symmetry is \(\frac{342}{175} \mathrm{Ma}^{2}\).

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The function $$ \Psi(r)=A\left(2-\frac{Z r}{a}\right) e^{-Z r / 2 a} $$ gives the form of the quantum mechanical wavefunction representing the electron in a hydrogen-like atom of atomic number \(Z\) when the electron is in its first allowed spherically symmetric excited state. Here \(r\) is the usual spherical polar coordinate, but, because of the spherical symmetry, the coordinates \(\theta\) and \(\phi\) do not appear explicitly in \(\Psi\). Determine the value that \(A\) (assumed real) must have if the wavefunction is to be correctly normalised, i.e. the volume integral of \(|\Psi|^{2}\) over all space is equal to unity.

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