The differential \(dV\) is \(dV=r^2\sin\theta\,d\theta\,d\phi\,dr\), so, \[\int\limits_{all\;space} |\psi|^2\;dV=\int\limits_{0}^{2\pi}\int\limits_{0}^{\pi}\int\limits_{0}^{\infty}\psi^*(r,\theta,\phi)\psi(r,\theta,\phi)\,r^2\sin\theta\,dr d\theta d\phi=1 \nonumber\]. This convention is used, in particular, for geographical coordinates, where the "zenith" direction is north and positive azimuth (longitude) angles are measured eastwards from some prime meridian. (25.4.6) y = r sin sin . We also knew that all space meant \(-\infty\leq x\leq \infty\), \(-\infty\leq y\leq \infty\) and \(-\infty\leq z\leq \infty\), and therefore we wrote: \[\int_{-\infty }^{\infty }\int_{-\infty }^{\infty }\int_{-\infty }^{\infty }{\left | \psi (x,y,z) \right |}^2\; dx \;dy \;dz=1 \nonumber\]. specifies a single point of three-dimensional space. , Where Now this is the general setup. $$ (b) Note that every point on the sphere is uniquely determined by its z-coordinate and its counterclockwise angle phi, $0 \leq\phi\leq 2\pi$, from the half-plane y = 0, PDF Concepts of primary interest: The line element Coordinate directions The straightforward way to do this is just the Jacobian. What Is the Difference Between 'Man' And 'Son of Man' in Num 23:19? Equivalently, it is 90 degrees (.mw-parser-output .sfrac{white-space:nowrap}.mw-parser-output .sfrac.tion,.mw-parser-output .sfrac .tion{display:inline-block;vertical-align:-0.5em;font-size:85%;text-align:center}.mw-parser-output .sfrac .num,.mw-parser-output .sfrac .den{display:block;line-height:1em;margin:0 0.1em}.mw-parser-output .sfrac .den{border-top:1px solid}.mw-parser-output .sr-only{border:0;clip:rect(0,0,0,0);height:1px;margin:-1px;overflow:hidden;padding:0;position:absolute;width:1px}/2 radians) minus the inclination angle. 10.2: Area and Volume Elements - Chemistry LibreTexts Total area will be $$r \, \pi \times r \, 2\pi = 2 \pi^2 \, r^2$$, Like this where \(a>0\) and \(n\) is a positive integer. The geometrical derivation of the volume is a little bit more complicated, but from Figure \(\PageIndex{4}\) you should be able to see that \(dV\) depends on \(r\) and \(\theta\), but not on \(\phi\). F & G \end{array} \right), We can then make use of Lagrange's Identity, which tells us that the squared area of a parallelogram in space is equal to the sum of the squares of its projections onto the Cartesian plane: $$|X_u \times X_v|^2 = |X_u|^2 |X_v|^2 - (X_u \cdot X_v)^2.$$ If the inclination is zero or 180 degrees ( radians), the azimuth is arbitrary. the orbitals of the atom). An area element "$d\phi \; d\theta$" close to one of the poles is really small, tending to zero as you approach the North or South pole of the sphere. Use your result to find for spherical coordinates, the scale factors, the vector d s, the volume element, and the unit basis vectors e r , e , e in terms of the unit vectors i, j, k. Write the g ij matrix. 14.5: Spherical Coordinates - Chemistry LibreTexts 16.4: Spherical Coordinates - Chemistry LibreTexts Cylindrical and spherical coordinates - University of Texas at Austin The wave function of the ground state of a two dimensional harmonic oscillator is: \(\psi(x,y)=A e^{-a(x^2+y^2)}\). , Therefore1, \(A=\sqrt{2a/\pi}\). In cartesian coordinates, all space means \(-\infty \underbrace {r \, d\theta}_{\text{longitude component}} *\underbrace {r \, \color{blue}{\sin{\theta}} \,d \phi}_{\text{latitude component}}}^{\text{area of an infinitesimal rectangle}} Is it possible to rotate a window 90 degrees if it has the same length and width? After rectangular (aka Cartesian) coordinates, the two most common an useful coordinate systems in 3 dimensions are cylindrical coordinates (sometimes called cylindrical polar coordinates) and spherical coordinates (sometimes called spherical polar coordinates ). , For a wave function expressed in cartesian coordinates, \[\int\limits_{all\;space} |\psi|^2\;dV=\int\limits_{-\infty}^{\infty}\int\limits_{-\infty}^{\infty}\int\limits_{-\infty}^{\infty}\psi^*(x,y,z)\psi(x,y,z)\,dxdydz \nonumber\]. Connect and share knowledge within a single location that is structured and easy to search. Accessibility StatementFor more information contact us atinfo@libretexts.orgor check out our status page at https://status.libretexts.org. Lets see how we can normalize orbitals using triple integrals in spherical coordinates. Volume element - Wikipedia conflicts with the usual notation for two-dimensional polar coordinates and three-dimensional cylindrical coordinates, where is often used for the azimuth.[3]. In the case of a constant or else = /2, this reduces to vector calculus in polar coordinates. 10.8 for cylindrical coordinates. The small volume we want will be defined by , , and , as pictured in figure 15.6.1 . This is shown in the left side of Figure \(\PageIndex{2}\). How to match a specific column position till the end of line? ( Calculating Infinitesimal Distance in Cylindrical and Spherical Coordinates , There is yet another way to look at it using the notion of the solid angle. If the radius is zero, both azimuth and inclination are arbitrary. Spherical Coordinates -- from Wolfram MathWorld Both versions of the double integral are equivalent, and both can be solved to find the value of the normalization constant (\(A\)) that makes the double integral equal to 1. where $B$ is the parameter domain corresponding to the exact piece $S$ of surface. Tool for making coordinates changes system in 3d-space (Cartesian, spherical, cylindrical, etc. Regardless of the orbital, and the coordinate system, the normalization condition states that: \[\int\limits_{all\;space} |\psi|^2\;dV=1 \nonumber\]. Another application is ergonomic design, where r is the arm length of a stationary person and the angles describe the direction of the arm as it reaches out. The volume element spanning from r to r + dr, to + d, and to + d is specified by the determinant of the Jacobian matrix of partial derivatives, Thus, for example, a function f(r, , ) can be integrated over every point in R3 by the triple integral. Relevant Equations: Surface integrals of scalar fields. In spherical polars, (g_{i j}) = \left(\begin{array}{cc} The result is a product of three integrals in one variable: \[\int\limits_{0}^{2\pi}d\phi=2\pi \nonumber\], \[\int\limits_{0}^{\pi}\sin\theta \;d\theta=-\cos\theta|_{0}^{\pi}=2 \nonumber\], \[\int\limits_{0}^{\infty}e^{-2r/a_0}\,r^2\;dr=? 4: The area shown in gray can be calculated from geometrical arguments as, \[dA=\left[\pi (r+dr)^2- \pi r^2\right]\dfrac{d\theta}{2\pi}.\]. I'm just wondering is there an "easier" way to do this (eg. The same value is of course obtained by integrating in cartesian coordinates. You have explicitly asked for an explanation in terms of "Jacobians". Blue triangles, one at each pole and two at the equator, have markings on them. The radial distance r can be computed from the altitude by adding the radius of Earth, which is approximately 6,36011km (3,9527 miles). The volume element is spherical coordinates is: The small volume is nearly box shaped, with 4 flat sides and two sides formed from bits of concentric spheres. In this case, \(n=2\) and \(a=2/a_0\), so: \[\int\limits_{0}^{\infty}e^{-2r/a_0}\,r^2\;dr=\dfrac{2! ( ) ( Because \(dr<<0\), we can neglect the term \((dr)^2\), and \(dA= r\; dr\;d\theta\) (see Figure \(10.2.3\)). We assume the radius = 1. The use of symbols and the order of the coordinates differs among sources and disciplines. Geometry Coordinate Geometry Spherical Coordinates Download Wolfram Notebook Spherical coordinates, also called spherical polar coordinates (Walton 1967, Arfken 1985), are a system of curvilinear coordinates that are natural for describing positions on a sphere or spheroid. $$S:\quad (u,v)\ \mapsto\ {\bf x}(u,v)$$ {\displaystyle (-r,\theta {+}180^{\circ },-\varphi )} In polar coordinates: \[\int\limits_{0}^{\infty}\int\limits_{0}^{2\pi} A^2 e^{-2ar^2}r\;d\theta dr=A^2\int\limits_{0}^{\infty}e^{-2ar^2}r\;dr\int\limits_{0}^{2\pi}\;d\theta =A^2\times\dfrac{1}{4a}\times2\pi=1 \nonumber\]. spherical coordinate area element = r2 Example Prove that the surface area of a sphere of radius R is 4 R2 by direct integration. The same situation arises in three dimensions when we solve the Schrdinger equation to obtain the expressions that describe the possible states of the electron in the hydrogen atom (i.e. Element of surface area in spherical coordinates - Physics Forums The azimuth angle (longitude), commonly denoted by , is measured in degrees east or west from some conventional reference meridian (most commonly the IERS Reference Meridian), so its domain is 180 180. r The spherical-polar basis vectors are ( e r, e , e ) which is related to the cartesian basis vectors as follows: Because of the probabilistic interpretation of wave functions, we determine this constant by normalization. 4: A cylindrical coordinate system is a three-dimensional coordinate system that specifies point positions by the distance from a chosen reference axis (axis L in the image opposite), the direction from the axis relative to a chosen reference direction (axis A), and the distance from a chosen reference plane perpendicular to the axis (plane containing the purple section). Both versions of the double integral are equivalent, and both can be solved to find the value of the normalization constant (\(A\)) that makes the double integral equal to 1. , It is because rectangles that we integrate look like ordinary rectangles only at equator! 10: Plane Polar and Spherical Coordinates, Mathematical Methods in Chemistry (Levitus), { "10.01:_Coordinate_Systems" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "10.02:_Area_and_Volume_Elements" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "10.03:_A_Refresher_on_Electronic_Quantum_Numbers" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "10.04:_A_Brief_Introduction_to_Probability" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "10.05:_Problems" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()" }, { "00:_Front_Matter" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "01:_Before_We_Begin" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "02:_Complex_Numbers" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "03:_Series" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "04:_First_Order_Ordinary_Differential_Equations" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "05:_Second_Order_Ordinary_Differential_Equations" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "06:_Power_Series_Solutions_of_Differential_Equations" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "07:_Fourier_Series" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "08:_Calculus_in_More_than_One_Variable" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "09:_Exact_and_Inexact_Differentials" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "10:_Plane_Polar_and_Spherical_Coordinates" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "11:_Operators" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "12:_Partial_Differential_Equations" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "13:_Determinants" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "14:_Vectors" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "15:_Matrices" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "16:_Formula_Sheets" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "zz:_Back_Matter" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()" }, [ "article:topic", "showtoc:no", "authorname:mlevitus", "differential volume element", "differential area element", "license:ccbyncsa", "licenseversion:40", "source@https://www.public.asu.edu/~mlevitus/chm240/book.pdf" ], https://chem.libretexts.org/@app/auth/3/login?returnto=https%3A%2F%2Fchem.libretexts.org%2FBookshelves%2FPhysical_and_Theoretical_Chemistry_Textbook_Maps%2FMathematical_Methods_in_Chemistry_(Levitus)%2F10%253A_Plane_Polar_and_Spherical_Coordinates%2F10.02%253A_Area_and_Volume_Elements, \( \newcommand{\vecs}[1]{\overset { \scriptstyle \rightharpoonup} {\mathbf{#1}}}\) \( \newcommand{\vecd}[1]{\overset{-\!-\!\rightharpoonup}{\vphantom{a}\smash{#1}}} \)\(\newcommand{\id}{\mathrm{id}}\) \( \newcommand{\Span}{\mathrm{span}}\) \( \newcommand{\kernel}{\mathrm{null}\,}\) \( \newcommand{\range}{\mathrm{range}\,}\) \( \newcommand{\RealPart}{\mathrm{Re}}\) \( \newcommand{\ImaginaryPart}{\mathrm{Im}}\) \( \newcommand{\Argument}{\mathrm{Arg}}\) \( \newcommand{\norm}[1]{\| #1 \|}\) \( \newcommand{\inner}[2]{\langle #1, #2 \rangle}\) \( \newcommand{\Span}{\mathrm{span}}\) \(\newcommand{\id}{\mathrm{id}}\) \( \newcommand{\Span}{\mathrm{span}}\) \( \newcommand{\kernel}{\mathrm{null}\,}\) \( \newcommand{\range}{\mathrm{range}\,}\) \( \newcommand{\RealPart}{\mathrm{Re}}\) \( \newcommand{\ImaginaryPart}{\mathrm{Im}}\) \( \newcommand{\Argument}{\mathrm{Arg}}\) \( \newcommand{\norm}[1]{\| #1 \|}\) \( \newcommand{\inner}[2]{\langle #1, #2 \rangle}\) \( \newcommand{\Span}{\mathrm{span}}\)\(\newcommand{\AA}{\unicode[.8,0]{x212B}}\), 10.3: A Refresher on Electronic Quantum Numbers, source@https://www.public.asu.edu/~mlevitus/chm240/book.pdf, status page at https://status.libretexts.org. Understand the concept of area and volume elements in cartesian, polar and spherical coordinates. This choice is arbitrary, and is part of the coordinate system's definition. The LibreTexts libraries arePowered by NICE CXone Expertand are supported by the Department of Education Open Textbook Pilot Project, the UC Davis Office of the Provost, the UC Davis Library, the California State University Affordable Learning Solutions Program, and Merlot. Why are Suriname, Belize, and Guinea-Bissau classified as "Small Island Developing States"? 4.3: Cylindrical Coordinates - Engineering LibreTexts Would we just replace \(dx\;dy\;dz\) by \(dr\; d\theta\; d\phi\)? Legal. PDF Math Boot Camp: Volume Elements - GitHub Pages Would we just replace \(dx\;dy\;dz\) by \(dr\; d\theta\; d\phi\)? This is shown in the left side of Figure \(\PageIndex{2}\). When using spherical coordinates, it is important that you see how these two angles are defined so you can identify which is which. You then just take the determinant of this 3-by-3 matrix, which can be done by cofactor expansion for instance. Area element of a surface[edit] A simple example of a volume element can be explored by considering a two-dimensional surface embedded in n-dimensional Euclidean space. The answer is no, because the volume element in spherical coordinates depends also on the actual position of the point. For the polar angle , the range [0, 180] for inclination is equivalent to [90, +90] for elevation. {\displaystyle m} ) \nonumber\], \[\int_{0}^{\infty}x^ne^{-ax}dx=\dfrac{n! ) Alternatively, we can use the first fundamental form to determine the surface area element. The blue vertical line is longitude 0. Spherical coordinates, Finding the volume bounded by surface in spherical coordinates, Angular velocity in Fick Spherical coordinates, The surface temperature of the earth in spherical coordinates. Spherical coordinates, also called spherical polar coordinates (Walton 1967, Arfken 1985), are a system of curvilinear coordinates that are natural for describing positions on a sphere or spheroid. This is the standard convention for geographic longitude. Figure 6.7 Area element for a cylinder: normal vector r Example 6.1 Area Element of Disk Consider an infinitesimal area element on the surface of a disc (Figure 6.8) in the xy-plane. A common choice is. The radial distance is also called the radius or radial coordinate. where we do not need to adjust the latitude component. $$ Here is the picture. r \[\int\limits_{0}^{2\pi}\int\limits_{0}^{\pi}\int\limits_{0}^{\infty}\psi^*(r,\theta,\phi)\psi(r,\theta,\phi) \, r^2 \sin\theta \, dr d\theta d\phi=\int\limits_{0}^{2\pi}\int\limits_{0}^{\pi}\int\limits_{0}^{\infty}A^2e^{-2r/a_0}\,r^2\sin\theta\,dr d\theta d\phi=1 \nonumber\], \[\int\limits_{0}^{2\pi}\int\limits_{0}^{\pi}\int\limits_{0}^{\infty}A^2e^{-2r/a_0}\,r^2\sin\theta\,dr d\theta d\phi=A^2\int\limits_{0}^{2\pi}d\phi\int\limits_{0}^{\pi}\sin\theta \;d\theta\int\limits_{0}^{\infty}e^{-2r/a_0}\,r^2\;dr \nonumber\]. AREA AND VOLUME ELEMENT IN SPHERICAL POLAR COORDINATES - YouTube In three dimensions, the spherical coordinate system defines a point in space by three numbers: the distance \(r\) to the origin, a polar angle \(\phi\) that measures the angle between the positive \(x\)-axis and the line from the origin to the point \(P\) projected onto the \(xy\)-plane, and the angle \(\theta\) defined as the is the angle between the \(z\)-axis and the line from the origin to the point \(P\): Before we move on, it is important to mention that depending on the field, you may see the Greek letter \(\theta\) (instead of \(\phi\)) used for the angle between the positive \(x\)-axis and the line from the origin to the point \(P\) projected onto the \(xy\)-plane. $g_{i j}= X_i \cdot X_j$ for tangent vectors $X_i, X_j$. $$ 1. In lieu of x and y, the cylindrical system uses , the distance measured from the closest point on the z axis, and , the angle measured in a plane of constant z, beginning at the + x axis ( = 0) with increasing toward the + y direction. $X(\phi,\theta) = (r \cos(\phi)\sin(\theta),r \sin(\phi)\sin(\theta),r \cos(\theta)),$ where \(a>0\) and \(n\) is a positive integer. In cartesian coordinates, the differential volume element is simply \(dV= dx\,dy\,dz\), regardless of the values of \(x, y\) and \(z\). Spherical coordinates (r, , ) as commonly used in physics ( ISO 80000-2:2019 convention): radial distance r (distance to origin), polar angle ( theta) (angle with respect to polar axis), and azimuthal angle ( phi) (angle of rotation from the initial meridian plane). thickness so that dividing by the thickness d and setting = a, we get { "32.01:_Complex_Numbers" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "32.02:_Probability_and_Statistics" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "32.03:_Vectors" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "32.04:_Spherical_Coordinates" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "32.05:_Determinants" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "32.06:_Matrices" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "32.07:_Numerical_Methods" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "32.08:_Partial_Differentiation" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "32.09:_Series_and_Limits" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "32.10:_Fourier_Analysis" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "32.11:_The_Binomial_Distribution_and_Stirling\'s_Appromixation" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()" }, { "00:_Front_Matter" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "01:_The_Dawn_of_the_Quantum_Theory" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "02:_The_Classical_Wave_Equation" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "03:_The_Schrodinger_Equation_and_a_Particle_in_a_Box" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "04:_Postulates_and_Principles_of_Quantum_Mechanics" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "05:_The_Harmonic_Oscillator_and_the_Rigid_Rotor" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "06:_The_Hydrogen_Atom" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "07:_Approximation_Methods" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "08:_Multielectron_Atoms" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "09:_Chemical_Bonding_in_Diatomic_Molecules" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "10:_Bonding_in_Polyatomic_Molecules" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "11:_Computational_Quantum_Chemistry" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "12:_Group_Theory_-_The_Exploitation_of_Symmetry" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "13:_Molecular_Spectroscopy" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "14:_Nuclear_Magnetic_Resonance_Spectroscopy" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "15:_Lasers_Laser_Spectroscopy_and_Photochemistry" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "16:_The_Properties_of_Gases" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "17:_Boltzmann_Factor_and_Partition_Functions" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "18:_Partition_Functions_and_Ideal_Gases" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "19:_The_First_Law_of_Thermodynamics" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "20:_Entropy_and_The_Second_Law_of_Thermodynamics" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "21:_Entropy_and_the_Third_Law_of_Thermodynamics" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "22:_Helmholtz_and_Gibbs_Energies" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "23:_Phase_Equilibria" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "24:_Solutions_I_-_Volatile_Solutes" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "25:_Solutions_II_-_Nonvolatile_Solutes" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "26:_Chemical_Equilibrium" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "27:_The_Kinetic_Theory_of_Gases" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "28:_Chemical_Kinetics_I_-_Rate_Laws" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "29:_Chemical_Kinetics_II-_Reaction_Mechanisms" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "30:_Gas-Phase_Reaction_Dynamics" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "31:_Solids_and_Surface_Chemistry" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "32:_Math_Chapters" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", Appendices : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "zz:_Back_Matter" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()" }, [ "article:topic", "showtoc:no", "license:ccbyncsa", "Spherical Coordinates", "autonumheader:yes2", "licenseversion:40" ], https://chem.libretexts.org/@app/auth/3/login?returnto=https%3A%2F%2Fchem.libretexts.org%2FBookshelves%2FPhysical_and_Theoretical_Chemistry_Textbook_Maps%2FPhysical_Chemistry_(LibreTexts)%2F32%253A_Math_Chapters%2F32.04%253A_Spherical_Coordinates, \( \newcommand{\vecs}[1]{\overset { \scriptstyle \rightharpoonup} {\mathbf{#1}}}\) \( \newcommand{\vecd}[1]{\overset{-\!-\!\rightharpoonup}{\vphantom{a}\smash{#1}}} \)\(\newcommand{\id}{\mathrm{id}}\) \( \newcommand{\Span}{\mathrm{span}}\) \( \newcommand{\kernel}{\mathrm{null}\,}\) \( \newcommand{\range}{\mathrm{range}\,}\) \( \newcommand{\RealPart}{\mathrm{Re}}\) \( \newcommand{\ImaginaryPart}{\mathrm{Im}}\) \( \newcommand{\Argument}{\mathrm{Arg}}\) \( \newcommand{\norm}[1]{\| #1 \|}\) \( \newcommand{\inner}[2]{\langle #1, #2 \rangle}\) \( \newcommand{\Span}{\mathrm{span}}\) \(\newcommand{\id}{\mathrm{id}}\) \( \newcommand{\Span}{\mathrm{span}}\) \( \newcommand{\kernel}{\mathrm{null}\,}\) \( \newcommand{\range}{\mathrm{range}\,}\) \( \newcommand{\RealPart}{\mathrm{Re}}\) \( \newcommand{\ImaginaryPart}{\mathrm{Im}}\) \( \newcommand{\Argument}{\mathrm{Arg}}\) \( \newcommand{\norm}[1]{\| #1 \|}\) \( \newcommand{\inner}[2]{\langle #1, #2 \rangle}\) \( \newcommand{\Span}{\mathrm{span}}\)\(\newcommand{\AA}{\unicode[.8,0]{x212B}}\), status page at https://status.libretexts.org.
Sammy The Bull New Podcast,
Tezfiles Link Generator,
Texas Labor Laws Doctor's Note,
Randy Mott Net Worth,
Mark Zuckerberg Has Made Significant Contributions To Society,
Articles A