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LSU Key.pngKey Equations

Whitworth's (1981) Isothermal Free-Energy Surface
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Each of the equations displayed in the Tables, below, encapsulates a physical concept that is fundamental to our understanding of — and, hence our discussion of — the structure, stability, and dynamics of self-gravitating fluids. The pervasiveness of these physical concepts throughout astrophysics is reflected in the fact that the same equations — perhaps written in slightly different forms — appear in numerous published books and research papers. When attempting to understand the physical concept that is associated with any one of these mathematical relations, it can be helpful to read how and in what context different authors have introduced the expression in their own work. These Tables offer guides to some parallel discussions that have appeared in published texts over the past 5+ decades in connection with selected sets of key physical relations.

EXAMPLE: Suppose you want to gain a better understanding of the origin of the ideal gas equation of state, the definition of the gas constant <math>~\Re</math>, or how to determine the value of the mean molecular weight <math>~\bar{\mu}</math> of a gas. According to the Table entitled Equations of State, you will find a discussion of the ideal gas equation of state: near Eq. (1) in §II.1 of Chandrasekhar (1967); near Eq. (80.8) in §IX.80 of Landau & Lifshitz (1975); near Eq. (5.91) in Vol. I, §5.6 of Padmanabhan (2000); etc. A "note" (linked to a comment further down on this page) appears along with a table entry if the relevant equation in the cited reference contains notations or symbol names that differ significantly from the equation as displayed here.

Principal Governing Equations

Principal Governing Equations

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Parallel References
§ no. and (Eq. no.)

Template_Name

Resulting Equation

C67

LL75

H87

ST83

KW94

P00

BLRY07

EQ_Continuity01

Continuity Equation:

LSU Key.png

<math>\frac{d\rho}{dt} + \rho \nabla \cdot \vec{v} = 0</math>

 

§I.1
(1.2)
Note

§5.4
(5.37)
Note

§6.1
(6.1.1)
Note

§2.5
(2.22)
Note

I: §8.5
(8.45)

§1.4
(1.53)

EQ_Euler01

Euler Equation:

LSU Key.png

<math>\frac{d\vec{v}}{dt} = - \frac{1}{\rho} \nabla P - \nabla \Phi</math>

 

§I.2
(2.1)
Note

§5.4
(5.38)
Note

§6.1
(6.1.2)

§2.5
(2.20)

I: §8.5
(8.48)

§1.4
(1.55)

EQ_FirstLaw01

1st Law of Thermodynamics:

LSU Key.png

<math>T \frac{ds}{dt} = \frac{d\epsilon}{dt} + P \frac{d}{dt} \biggl(\frac{1}{\rho}\biggr)</math>

 

§I.2
(2.5)
Note

§4.2
(4.31)
Note

§6.1
(6.1.8)

§4.1
(4.1)
Note

I: §8.5
(8.53)

 

EQ_Poisson01

Poisson Equation:

LSU Key.png

<math>\nabla^2 \Phi = 4\pi G \rho</math>

 

§I.3
(3.5)
Note

 

§6.1
(6.1.4)

§1.3
(1.9)

I: §10.2
(10.1)
Note

Chap. 7

Equations of State

Equations of State

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Parallel References
§ no. and (Eq. no.)

Template_Name

Resulting Equation

C67

LL75

H87

ST83

KW94

P00

BLRY07

EQ_EOSideal0A

Ideal Gas Equation of State:

LSU Key.png

<math>~P_\mathrm{gas} = \frac{\Re}{\bar{\mu}} \rho T</math>

§II.1
(1)
Note

§IX.80
(80.8)
Note

§1.1
("n")

§2.3
(2.3.32)
or
(3.2.12)

§13.0
(13.1)
Note

I: §5.6
(5.91)

§5.4
(5.34)

EQ_ZTFG01

Degenerate Electron Pressure:

LSU Key.png

<math>~P_\mathrm{deg} = A_\mathrm{F} F(\chi) </math>

where:  <math>F(\chi) \equiv \chi(2\chi^2 - 3)(\chi^2 + 1)^{1/2} + 3\sinh^{-1}\chi</math>

and:   

<math>\chi \equiv (\rho/B_\mathrm{F})^{1/3}</math>


 

———   NOTE:   ———
<math> F(\chi) = \frac{8}{5}\chi^5 - \frac{4}{7}\chi^7 + \cdots ~~~~~~(\mathrm{for}~~ \chi\ll 1) </math>

<math> F(\chi) = 2\chi^4 - 2\chi^2 + \cdots ~~~~~~~(\mathrm{for}~~ \chi\gg 1) </math>

§X.1
(19)
+
(20)

 

§11.2
(11.41)

§2.3
(2.3.5)
+
(2.3.6)

§15.0
(15.13)
+
(15.14)

I: §5.9.2
(5.156)
+
(5.158)

§5.6.1
(5.86)
+
(5.87)
+
(5.88)

EQ_EOSradiation01

Radiation Pressure:

LSU Key.png

<math>~P_\mathrm{rad} = \frac{1}{3} a_\mathrm{rad} T^4</math>

 

 

§12.1
(12.12)
+
(12.15)

 

 

 

§5.6.1
(5.85)

EQ_PressureTotal01

Normalized Total Pressure:

LSU Key.png

<math>~p_\mathrm{total} = \biggl(\frac{\mu_e m_p}{\bar{\mu} m_u} \biggr) 8 \chi^3 \frac{T}{T_e} + F(\chi) + \frac{8\pi^4}{15} \biggl( \frac{T}{T_e} \biggr)^4</math>

 

 

 

 

 

 

 

Traditional Equations of (Spherical) Stellar Structure

Traditional Equations of (Spherical) Stellar Structure

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Parallel References
§ no. and (Eq. no.)

Template_Name

Resulting Equation

C67

LL75

H87

ST83

KW94

P00

BLRY07

EQ_SSmassConservation01

Mass Conservation:

LSU Key.png

<math>~\frac{dM_r}{dr} = 4\pi r^2 \rho</math>

§IV.2
(6)

 

 

§3.2
(3.2.1)

§9.1
(9.1)

II: §2.2
(2.23)

§5.1
(5.2)

EQ_SShydrostaticBalance01

Hydrostatic Balance:

LSU Key.png

<math>~\frac{dP}{dr} = - \frac{GM_r \rho}{r^2}</math>

§IV.2
(6)

 

 

§3.2
(3.2.2)

§9.1
(9.2)
Note

II: §2.2
(2.22)

§5.1
(5.1)

EQ_SSLaneEmden01

Polytropic Lane-Emden Equation:

LSU Key.png

<math>~\frac{1}{\xi^2} \frac{d}{d\xi}\biggl( \xi^2 \frac{d\Theta_H}{d\xi} \biggr) = - \Theta_H^n</math>


Emden (1907)
Ritter (1880)

§IV.2
(11)
Note

 

 

§3.3
(3.3.6)

§19.2
(19.10)

I: §10.3
(10.4)

 

EQ_SSLaneEmden02

Isothermal Lane-Emden Equation:

LSU Key.png

<math>~\frac{1}{\xi^2} \frac{d}{d\xi}\biggl( \xi^2 \frac{d\psi}{d\xi} \biggr) = e^{-\psi}</math>


§IV.22
(374)

 

 

 

§19.8
(19.35)

I: §10.3.3
(10.23)

 

 

Stability: Radial Pulsation

Stability: Radial Pulsation

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Parallel References
§ no. and (Eq. no.)

Template_Name

Resulting Equation

C67

ST83

KW94

HK99

P00

EQ_RadialPulsation01

LAWE:   Linear Adiabatic Wave (or Radial Pulsation) Equation

LSU Key.png

<math>~ \frac{d^2x}{dr_0^2} + \biggl[\frac{4}{r_0} - \biggl(\frac{g_0 \rho_0}{P_0}\biggr) \biggr] \frac{dx}{dr_0} + \biggl(\frac{\rho_0}{\gamma_\mathrm{g} P_0} \biggr)\biggl[\omega^2 + (4 - 3\gamma_\mathrm{g})\frac{g_0}{r_0} \biggr] x = 0 </math>


Eddington (1926)

 

§6.5
(6.5.6)

§38.1
(38.8)

§10.1.1
(10.16)

II: §3.7.1
(3.144)

EQ_RadialPulsation02

Polytropic LAWE:

LSU Key.png

<math>~0 = \frac{d^2x}{d\xi^2} + \biggl[ 4 - (n+1) Q \biggr] \frac{1}{\xi} \cdot \frac{dx}{d\xi} + (n+1) \biggl[ \biggl( \frac{\sigma_c^2}{6\gamma_g } \biggr) \frac{\xi^2}{\theta} - \alpha Q\biggr] \frac{x}{\xi^2} </math>

where:    <math>~Q(\xi) \equiv - \frac{d\ln\theta}{d\ln\xi} \, ,</math>    <math>~\sigma_c^2 \equiv \frac{3\omega^2}{2\pi G\rho_c} \, ,</math>     and,     <math>~\alpha \equiv \biggl(3 - \frac{4}{\gamma_\mathrm{g}}\biggr)</math>


 

 

 

 

 

EQ_RadialPulsation03

Isothermal LAWE:

LSU Key.png

<math>~0 = \frac{d^2x}{d\xi^2} + \biggl[4 - \xi \biggl( \frac{d\psi}{d\xi} \biggr) \biggr] \frac{1}{\xi} \cdot \frac{dx}{d\xi} + \biggl[ \biggl( \frac{\sigma_c^2}{6\gamma_\mathrm{g}}\biggr)\xi^2 - \alpha \xi \biggl( \frac{d\psi}{d\xi} \biggr) \biggr] \frac{x}{\xi^2} </math>

where:    <math>~\sigma_c^2 \equiv \frac{3\omega^2}{2\pi G\rho_c}</math>     and,     <math>~\alpha \equiv \biggl(3 - \frac{4}{\gamma_\mathrm{g}}\biggr)</math>


 

 

 

 

 

 

Special Function Relationships

Gamma Function

Gamma Function

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Resulting Equation

EQ_Gamma01

LSU Key.png

<math>~ \Gamma(z) ~\Gamma(1-z) </math>

<math>~=</math>

<math>~ \frac{\pi}{\sin(\pi z)} </math>

<math>~\biggl|</math>

for example, if
<math>~z \rightarrow (m-n + \tfrac{1}{2})</math>

<math>~\Rightarrow ~~~\Gamma(m-n+\tfrac{1}{2})~\Gamma(n-m+\tfrac{1}{2})</math>

<math>~=</math>

<math>~\pi \biggl\{\sin\biggl[ \frac{\pi}{2} + \pi(m-n) \biggr] \biggr\}^{-1}</math>

 

<math>~=</math>

<math>~\pi (-1)^{m-n} </math>

DLMF §5.5(ii)

<math>~\biggl|</math>
Valid for:

   <math>~z \ne0, \pm 1, \pm 2, </math> …

<math>~\biggl|</math>


Toroidal Function Evaluations

Toroidal Function Evaluations

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Graphical Representation
(see:  generic caption)

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Resulting Equation

EQ_PminusHalf01

LSU Key.png

<math>~P_{-\frac{1}{2}}(z)</math>

<math>~=</math>

<math>~ \frac{2}{\pi} \biggl[\frac{2}{z+1}\biggr]^{1 / 2} ~K\biggl( \sqrt{ \frac{z-1}{z+1}} \biggr) </math>

      for example …

<math>~P_{-\frac{1}{2}}(\cosh\eta)</math>

<math>~=</math>

<math>~ \biggl[ \frac{\pi}{2} \cdot \cosh \frac{\eta}{2} \biggr]^{-1} K\biggl( \tanh \frac{\eta}{2} \biggr) </math>

Abramowitz & Stegun (1995), p. 337, eq. (8.13.1)

Abramowitz & Stegun (1995), p. 337, eq. (8.13.2)

P0minusHalf

EQ_QminusHalf01

LSU Key.png

<math>~Q_{-\frac{1}{2}}(z)</math>

<math>~=</math>

<math>~ \sqrt{ \frac{2}{z+1} } ~K\biggl( \sqrt{ \frac{2}{z+1}} \biggr) </math>

      for example …

<math>~Q_{-\frac{1}{2}}(\cosh\eta)</math>

<math>~=</math>

<math>~ 2 e^{-\eta/2} K(e^{-\eta}) </math>

Abramowitz & Stegun (1995), p. 337, eq. (8.13.3)

Abramowitz & Stegun (1995), p. 337, eq. (8.13.4)

P0minusHalf

EQ_PplusHalf01

LSU Key.png

<math>~P_{+ \frac{1}{2}}(z)</math>

<math>~=</math>

<math>~ \frac{2}{\pi} \biggl[z + \sqrt{ z^2-1} \biggr]^{1 / 2} ~E\biggl( \sqrt{ \frac{2(z^2-1)^{1 / 2}}{z + (z^2-1)^{1 / 2}}} \biggr) </math>

      for example …

<math>~P_{+ \frac{1}{2}}(\cosh\eta)</math>

<math>~=</math>

<math>~ \frac{2}{\pi}~e^{\eta/2}~ E( \sqrt{1-e^{-2\eta}} ) </math>

Abramowitz & Stegun (1995), p. 337, eq. (8.13.5)

Abramowitz & Stegun (1995), p. 337, eq. (8.13.6)

P0plusHalf

EQ_QplusHalf01

LSU Key.png

<math>~Q_{+\frac{1}{2}}(z)</math>

<math>~=</math>

<math>~ z \sqrt{ \frac{2}{z+1} }~K\biggl( \sqrt{ \frac{2}{z+1} } \biggr) ~-~ [2(z+1)]^{1 / 2} E\biggl( \sqrt{ \frac{2}{z+1} } \biggr) </math>

Abramowitz & Stegun (1995), p. 337, eq. (8.13.7)

P0plusHalf

EQ_Q1minusHalf01

LSU Key.png

<math>~Q^1_{-\frac{1}{2}}(z)</math>

<math>~=</math>

<math>~ - \biggl[\frac{1}{2(z-1)} \biggr]^{1 / 2} E(k) </math>

where:   <math>~k = \sqrt{ \frac{2}{z+1}} \, .</math>

(see our associated derivation)

ABSQ1minusHalf

EQ_Q2minusHalf01

LSU Key.png

<math>~Q^2_{-\frac{1}{2}}(z)</math>

<math>~=</math>

<math>~ \frac{ 4 z E(k) - (z-1) K(k) }{ [2^{3} (z+1) (z-1)^{2} ]^{1 / 2}} </math>

where:   <math>~k \equiv \sqrt{ \frac{2}{z+1}} \, .</math>

(see our associated derivation)

Q2minusHalf


Caption for Plots:   Here we explain how we assembled the various plots — shown immediately above in the right-hand column of the "Toroidal Function Evaluations" table — that depict the behavior of various associated Legendre (toroidal) functions (see the related discussion) having varying half-integer degrees <math>~P^0_{-\frac{1}{2}}</math>, <math>~P^0_{+\frac{1}{2}}</math>, <math>~Q^0_{-\frac{1}{2}}</math>, <math>~Q^0_{+\frac{1}{2}}</math>, <math>~Q^0_{+\frac{3}{2}} \, ,</math> and (in association with a separate related discussion) having varying order <math>~Q^1_{-\frac{1}{2}}</math>, <math>~Q^2_{-\frac{1}{2}}</math>.


For each choice of the integer indexes, <math>~n \ge 0</math> and <math>~m \ge 0</math>, the relevant plot shows how the function, <math>~X^n_{m-\frac{1}{2}}(z)</math>, varies with <math>~z</math>. The solid green circular markers in each plot identify data that has been pulled directly from Table IX (p. 1923) of [MF53]. In each plot, the solid orange circular markers identify function values that we have calculated using the relevant formulae as expressed herein in terms of the complete elliptic integrals, <math>~K(k)</math> and <math>~E(k)</math>, where the relevant values of the elliptic integrals have been pulled directly from tabulated values published in pp. 535 - 537 of the 1971 (19th) edition of the CRC's Standard Mathematical Tables, published by the Chemical Rubber Co., Cleveland, Ohio, U.S.A..


NOTE: The tabulated values of the function, <math>~Q^1_{-\frac{1}{2}}</math>, that appear in Table IX (p. 1923) of [MF53] are all positive, whereas, according to our derivation, they should all be negative. Therefore, for comparison purposes of this specific function — both here and in our accompanying discussion — we have plotted the absolute value of the function, <math>~|Q^1_{-\frac{1}{2}}(z)|</math>.


ADDITIONAL NOTE:   In Example 4 on p. 340 of Abramowitz & Stegun (1995), we can pull one additional data point for comparison; specifically, they provide a high-precision evaluation of <math>~Q^0_{-\frac{1}{2}}(z = 2.6) = 1.419337751</math>, which is entirely consistent with the lower-precision value that we have extracted from [MF53].


Relationships Between Various Associated Legendre Functions

Relationships Between Various Associated Legendre Functions

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Resulting Equation

EQ_Toroidal01

LSU Key.png

<math>~ Q_\nu[t t^' - (t^2-1)^{1 / 2} (t^{'2} - 1)^{1 / 2} \cos\psi] </math>

<math>~=</math>

<math>~ Q_\nu(t) P_\nu(t^') + 2\sum_{n=1}^\infty (-1)^n Q^n_\nu(t) P^{-n}_\nu(t^') \cos(n\psi) </math>

A. Erdélyi (1953):  Volume I, §3.11, p. 169, eq. (4)

Valid for:    

<math>~t, t^'</math>  real

       

<math>~1 < t^' < t</math>

       

<math>~\nu \ne -1, -2, -3, </math> …

       

<math>~\psi</math>   real

EQ_Toroidal02

LSU Key.png

<math>~Q_{n-1 / 2}^m (\lambda)</math>

<math>~=</math>

<math>~(-1)^n \frac{\pi^{3/2}}{\sqrt{2}~ \Gamma(n-m+1 / 2)} (x^2-1)^{1 / 4} P_{m-1 / 2}^n(x) \, , </math>

Gil, Segura, & Temme (2000):  eq. (8)

where:    

<math>~\lambda \equiv x/\sqrt{x^2-1}</math>

EQ_Toroidal03

LSU Key.png

<math>~Q_\nu^\mu(z)</math>

<math>~=</math>

<math>~ e^{i \mu \pi} ~ (2\pi)^{-\frac{1}{2}} (z^2-1)^{\mu/2} ~\Gamma(\mu + \tfrac{1}{2})~\biggl\{ \int_0^\pi (z - \cos t)^{-\mu - \frac{1}{2}} \cos[(\nu + \tfrac{1}{2})t] ~dt -\cos(\nu\pi) \int_0^\infty (z + \cosh t)^{-\mu - \frac{1}{2}} e^{-(\nu + \frac{1}{2})t} ~dt \biggr\} </math>

A. Erdélyi (1953):  Volume I, §3.7, p. 156, eq. (10)

Valid for:    

<math>~\mathrm{Re} ~\nu > -\tfrac{1}{2}</math> 

    and    

<math>~\mathrm{Re} (\nu + \mu + 1) > 0 \, .</math>

 

EQ_Toroidal04

LSU Key.png

<math>~(\nu - \mu + 1)P^\mu_{\nu + 1} (z)</math>

<math>~=</math>

<math>~ (2\nu + 1)z P_\nu^\mu(z) - (\nu + \mu)P^\mu_{\nu-1}(z) </math>

Abramowitz & Stegun (1995), p. 334, eq. (8.5.3)

NOTE: <math>~Q_\nu^\mu</math>, as well as <math>~P_\nu^\mu</math>, satisfies this same recurrence relation.

EQ_Toroidal05

LSU Key.png

<math>~ \int_a^b\biggl[(\nu - \sigma)(\nu + \sigma + 1) + (\rho^2 - \mu^2)(1 - z^2)^{-1} \biggr] w_\nu^\mu ~w_\sigma^\rho ~dz </math>

<math>~=</math>

<math>~ \biggl[ z(\nu-\sigma) w_\nu^\mu ~w_\sigma^\rho + (\sigma+\rho) w_\nu^\mu ~ w_{\sigma-1}^\rho - (\nu + \mu) w_{\nu - 1}^\mu ~w_\sigma^\rho \biggr]_a^b </math>

A. Erdélyi (1953):  Volume I, §3.12, p. 169, eq. (1)

where, <math>~w_\nu^\mu(z)</math> and <math>~w_\sigma^\rho(z)</math> denote any solutions of Legendre's differential equation

EQ_Toroidal06

LSU Key.png

<math>~(\xi - z)\sum_{m=0}^n (2m+1)P_m(z) Q_m(\xi)</math>

<math>~=</math>

<math>~ 1 - (\ell+1)[P_{\ell+1}(z) Q_\ell(\xi) - P_\ell(z)Q_{\ell+1}(\xi)] </math>

Abramowitz & Stegun (1995), p. 335, eq. (8.9.2)

EQ_Toroidal07

LSU Key.png

<math>~P_\nu^{\mu + 1}(z)</math>

<math>~=</math>

<math>~ (z^2-1)^{-\frac{1}{2}} \{ (\nu - \mu) z P^\mu_\nu(z) - (\nu + \mu)P^\mu_{\nu - 1}(z)\} </math>

Abramowitz & Stegun (1995), p. 333, eq. (8.5.1)

NOTE: <math>~Q_\nu^\mu</math>, as well as <math>~P_\nu^\mu</math>, satisfies this same recurrence relation.

 

Key Parallel References (printed texts spanning 5+ decades)

  • [C67] Chandrasekhar, S. 1967 (originally, 1939), An Introduction to the Study of Stellar Structure (New York: Dover)
    • EQ_EOSideal0A — In C67, the ideal gas equation of state is initially written in terms of the specific volume <math>~V</math>, instead of the mass density <math>~\rho</math>; also, it is initially assumed that <math>~\bar{\mu}</math> = 1. Both <math>~\rho</math> and <math>~\bar{\mu}</math> are introduced in §III.1, Eq.(5).
    • EQ_SSLaneEmden01 — At the end of his Chapter IV, C67 writes an extensive history of the earliest work on stellar structure pointing especially the origins of the so-called Lane-Emden equation. He points out, for example, that Ritter (1880) actually published this governing differential equation prior to Emden.


  • [LL75] Laundau, L. D. & Lifshitz, E. M. 1975 (originally, 1959), Fluid Mechanics (New York: Pergamon Press)
    • EQ_Continuity01 — LL75 present the Eulerian, rather than the Lagrangian form of the Continuity equation.
    • EQ_Euler01 — In the Euler equation, LL75 do not initially include a source term to account for a gradient in the Newtonian gravitational potential, <math>~\Phi</math>; a term representing acceleration due to gravity, <math>\vec{g} = -\nabla\Phi</math>, is introduced in Eq.(2.4), but in LL75 this is intended primarily to describe gravity at the surface of the Earth.
    • EQ_FirstLaw01 — LL75's Eq.(2.5) must be combined with their discussion of what they refer to as the familiar thermodynamic relation (between LL75 Eqs. 2.8 and 2.9) in order to appreciate the similarity with our expression.
    • EQ_Poisson01 — In LL75, the symbol <math>\Delta</math>, rather than <math>\nabla^2</math>, is used to represent the Laplacian spatial operator.
    • EQ_EOSideal0A — In LL75, the ideal gas equation of state is written in terms of the specific volume <math>~V</math>, as well as in terms of the mass density <math>~\rho</math>.


  • [ST83] Shapiro, S. L. & Teukolsky, S. A. 1983, Black Holes, White Dwarfs, and Neutron Stars: The Physics of Compact Objects (New York: John Wiley & Sons); republished in 2004 by WILEY-VCH Verlag GmbH & Co. KGaA
    • EQ_Continuity01 — ST83 present the Eulerian, rather than the Lagrangian form of the Continuity equation.


  • [H87] Huang, K. 1987 (originally 1963), Statistical Mechanics (New York: John Wiley & Sons)
    • EQ_Continuity01 — H87 presents the Eulerian, rather than the Lagrangian form of the Continuity equation, and the variable <math>\vec{u}</math> is used instead of <math>~\vec{v}</math> to represent the velocity.
    • EQ_Euler01 — H87 presents the Eulerian, rather than the Lagrangian form of the Euler equation, and the variable <math>\vec{u}</math> is used instead of <math>~\vec{v}</math> to represent the velocity. Furthermore, to match the source term in our version of the Euler equation, we must set H87's applied acceleration, <math>\vec{F}/m = -\nabla</math><math>~\Phi</math>.
    • EQ_FirstLaw01 — H87 begins a discussion of the 1st Law of Thermodynamics in the first section of the first chapter, but it does not appear in the form we present (relevant for a "dilute gas") until Eq.(4.31).


  • [BT87] Binney, J. & Tremaine, S. 1987, Galactic Dynamics (Princeton, NJ: Princeton University Press)


  • [KW94] Kippenhahn, R. & Weigert, A. 1994, Stellar Structure and Evolution (New York: Springer-Verlag)
    • EQ_Continuity01 — KW94 present the Eulerian, rather than the Lagrangian form of the Continuity equation.
    • EQ_FirstLaw01 — In KW94, the symbol <math>u</math> instead of <math>~\epsilon</math> is used to represent the specific internal energy.
    • EQ_EOSideal0A — In KW94, the ideal gas equation of state is actually first introduced in §2.2, Eq.(27), but it is seriously discussed in Chapter 13. KW94 provide a particularly nice explanation of how to calculate the model parameter, <math>~\bar{\mu}</math>.
    • EQ_SShydrostaticBalance01 — In KW94, the hydrostatic balance equation is expressed in terms of <math>dP/dM_r</math> instead of <math>dP/dr</math>; and the second term on the right-hand-side allows for a net radial acceleration.


  • [HK99] Hansen, C. J. & Kawaler, S. D. 1999, Stellar Interiors: Physical Principles, Structure, and Evolution (New York: Springer)


  • [P00] Padmanabhan, T. 2000, Theoretical Astrophysics. Volume I: Astrophysical Processes (Cambridge: Cambridge University Press); and Padmanabhan, T. 2001, Theoretical Astrophysics. Volume II: Stars and Stellar Systems (Cambridge: Cambridge University Press)
    • EQ_Poisson01 — See also Vol.I: §10.4, Eq.(10.58).


  • [BLRY07] Bodenheimer, P., Laughlin, G. P., Różyczka, M. & Yorke, H. W. 2007, Numerical Methods in Astrophysics An Introduction (New York: Taylor & Francis)

Other Equations with Assigned Templates

To insert a given equation into any Wiki document, type ...
{{ User:Tohline/Math/Template_Name }}

Template_Name

Resulting Equation

Description

EQ_Continuity02

<math>~\frac{\partial\rho}{\partial t} + \nabla \cdot (\rho \vec{v}) = 0</math>

Eulerian (and Conservative) form of the continuity equation.

EQ_Euler02

<math>~\frac{\partial\vec{v}}{\partial t} + (\vec{v}\cdot \nabla) \vec{v}= - \frac{1}{\rho} \nabla P - \nabla \Phi</math>

Eulerian form of the Euler equation.

EQ_Euler03

<math>~\frac{\partial(\rho\vec{v})}{\partial t} + \nabla\cdot [(\rho\vec{v})\vec{v}]= - \nabla P - \rho \nabla \Phi</math>

Conservative form of the Euler equation.

EQ_Euler04

<math>~\frac{\partial\vec{v}}{\partial t} + \vec\zeta \times \vec{v}= - \frac{1}{\rho} \nabla P - \nabla \biggl[\Phi + \frac{1}{2}v^2 \biggr] </math>

Euler equation in terms of vorticity.

EQ_FirstLaw02

<math>~\frac{d\epsilon}{dt} + P \frac{d}{dt} \biggl(\frac{1}{\rho}\biggr) = 0</math>

Adiabatic form of the 1st Law of Thermodynamics.

EQ_Polytrope01

<math>~P = K_\mathrm{n} \rho^{1+1/n}</math>

Polytropic equation of state.

EQ_Polytrope02

<math>~H = (n+1)K_\mathrm{n} \rho^{1/n}</math>

Enthalpy in a polytrope.

EQ_Polytrope03

<math>~\rho = \biggl[ \frac{H}{(n+1)K_\mathrm{n}} \biggr]^n </math>

Density in terms of enthalpy for polytrope.

EQ_EOSideal00

<math>~P = n_g k T</math>

Alternate form of the ideal gas equation of state.

EQ_EOSideal02

<math>~P = (\gamma_\mathrm{g} - 1)\epsilon \rho </math>

Alternate form of the ideal gas equation of state.

EQ_TRApproximation

LSU Key.png

<math>~\Phi_\mathrm{TR}(\varpi,z)</math>

<math>~=</math>

<math>~-\biggl[ \frac{2GM}{\pi } \biggr]\frac{K(k)}{\sqrt{(\varpi+a)^2 + z^2}}</math>

<math>\mathrm{where:}~~~k \equiv \{4\varpi a/[ (\varpi+a)^2 + z^2]\}^{1 / 2}</math>

Gravitational potential exterior to an axisymmetric torus,
in the Thin Ring (TR) Approximation.

 


 

Whitworth's (1981) Isothermal Free-Energy Surface

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