Semester 1 - Formulas Flashcards

1
Q

Gravity

A

g(r) = Gm(r)/r^2

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2
Q

Hydrostatic Equilibrium

A

dP/dr = -p(r)g(r)

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3
Q

Gravitational Potential Energy

A

Ω = -GM^2/R

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4
Q

number density

A

n = p/mH

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5
Q

Mass

A

M = Vp

M = 4/3 πR^3 p

M = ( R ∫ 0) dm(r)

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6
Q

Core Pressure

A

P(c) = P(gas,i) + P(deg,e)

i = ions
e = electrons

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7
Q

Adiabatic Index

A

gamma = 1 + 1/n

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8
Q

Mean Free Path Derivation

A

s(bar) = l1(bar) + l2(bar) + l3(bar) + … + lN(bar)

s^2 = Nl^2

t = l/c

l = 1/nσ

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9
Q

Mean Free Path

A

l = 1/nσ

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10
Q

Gas Pressure

A

Pg = nkT

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11
Q

Radiation Pressure

A

Prad = 1/3 aT^4

a = 4σ/c

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12
Q

Degeneracy Pressure (non-relativistic and relativistic)

A

P = Kn^5/3 (non-relativistic)

P = Kn^4/3 (relativistic)

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13
Q

characteristic energy-loss timescale

A

τ = E/L

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14
Q

kelvin-helmholtz timescale

A

τ = Ω/L

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15
Q

potential energy of a star

A

m(r) = ( r ∫ 0) dm

if m = 4/3πr^3 p

dm = 4πp(r)r^2dr

Ω = - ( M* ∫ 0) Gm(r)dm/r

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16
Q

hydrostatic equilibrium derivation

A

A[P(r) - P(r+∆r)] - g(r)p(r)A∆r = 0

Taylor expand P(r+∆r)

P(r) + dP/dr ∆r + …

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17
Q

free-fall timescale derivation

A

a = dv/ dt = -Gm/r^2

dv/dt = 1/2 dv^2/dr

integrate and solve for v

free fall timescale = (0 ∫ r0) dt/dr dr

substitute in 1/v , change variables x = r/r0 and integrate

x = sin^2 theta => pi^2/4

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18
Q

Virial Theorem Derivation

A

start from hydrostatic equilibrium

multiply both sides by volume and integrate over r

RHS

dm = 4πr^2pdr

Ω = (M ∫ 0) Gmdm/r

LHS

integrate by parts at R, P=0

dm = 4πr^2pdr

  • (V ∫ 0) PdV

P = nkT

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19
Q

mean atomic mass

A

1/µi = Σj Xj/Aj

where Xj is the fraction by mass
and Aj its atomic weight

20
Q

the average number of free electrons per nucleon

A

1/µe = Σj Xjqj/Aj

where qj is the no. of free electrons per nucleon

21
Q

mean molecular mass

A

1/µ = 1/µi + 1/µe

22
Q

minimum stellar mass

23
Q

polytropic model

A

P = Kp^(gamma)

24
Q

lane-emden equation derivation

A

star from H.E. rearranged for m

insert dm/dr for m (include d/dr) and substitute polytropic relationship

dP/dr = dP/dp dp/dr chain rule

trial solutions of the form p = pcθ^n

chain rule

adiabatic index = 1 + 1/n

Const = alpha ^2

25
opacity
dτv = -kvpIvds
26
Rosseland mean opacity
F = ( ∞ ∫ 0) Fvdv Fvkvp/c = -dPv/dr and Pv = 4π/3c Bv dBv/dT dT/dr
27
kramers opacity
κ = κ0 p^pT^q
28
Coloumb repulsion
kbTign > z1z2e^2/4π εr
29
Eddington quartic equation
1-β = 0.003(M/Msun)^2 µ^4β^4
30
Number density
n = 2 electron density
31
Volume of shell
4πr^2dr
32
Energy release rate from the P-P chain
ε = p^2 T^4
33
Energy release rate for CNO-cycle
ε = p^2 T^16
34
Main branch of the P-P chain
PP-1 p+ + p+ -> 2H + e+ + v 2H + p+ -> 3He + gamma 3He + 3He -> 4He + 2p+
35
Temperature gradient derivation
P = Kp^gamma and P = pkT/mumH p = PmumH/kT insert p into P = p^gamma Take derivative with respect to r Eventually giving the temperate gradient
36
A star that is stable against convection
dT/dr|star < dT/dr|temp gradient (adiabatic) where gamma = 5/3 for non relativistic
37
A uniform density
p = p0 and p0 = M/4/3piR^3
38
Mass luminosity relationship
L*/Lsun =(M*/Msun)^3.5
39
To find the slope of the main sequence
Looking for the log relationship of L and Teff
40
If p(r) = constant than alpha = 3/5 for the potential energy.
Start from definition of potential energy. Ω = ∫ Gmdm/r Substitute dm and m(r) assuming uniform density integrate for r
41
Show

~ GM^2/R^4

Ω/3 = -

V substitute for Ω

42
Derive the temperature in a contracting protostar
Pc = Pg + PD replace n with p = nmH and assume μ = 1 Pc ~ GM^2/R^4 = 𝜒 GM^2/R^4 rearrange for kTc remember to divide both sides. pc = 𝛽 M/R^3 find R^4 and replace kbTc = Apc^1/3 - Bpc^2/3 find the minimum M by taking derivative which gives max T.
43
Derive the radiation pressure
L = (inf int 0) Lv dv Fv = Lv/4𝜋𝑟^2 p = hv/c Hence = L/4𝜋𝑟^2𝑐
44
Lower limit for the central core pressure
dP/dr = -pg dP/dm = -Gm/4pir^4 integrate between M* and 0 where r < R* Pc - Psurf > GM^2/8piR^4 and Psurf > 0
45
Show that Pv = 4π/3c Bv If P = 1/3 (∞ ∫ 0) pvn(p) dp
p = hv/c and v -> c in P n(v) = 4πBv/hvc Prad = (∞ ∫ 0) Pv dv Pv = 4π/3c Bv
46
Derive the temperature gradient in the case of radiative transport
F = ∫ Fv dv where Fv = -c/kp dP/dr dP/dT dT/dr = dP/dr dPrad = aT^4/3 so dP/dT = 4aT^3/3 and F = L/4πr^2
47
Derive the Eddington quartic equation
𝜅𝜂 ≈ const ≡ 𝜅𝑠 dPrad/dP = 𝐿𝜅/4𝜋𝑐𝐺𝑚 Integrate 𝛽 =𝑃𝑔𝑎𝑠/𝑃 (1-𝛽) =𝑃rad/𝑃 Prad = aT^4/3 and assuming the ideal gas law we can rearrange for T Substituting constants for Eddington quartic equation