Semester 1 - Formulae Flashcards

1
Q

Number of stars per unit volume

A

N = ∫ ndV

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2
Q

Volume element of a sphere

A

dV = r^2 sinθdrdθdΦ

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3
Q

Galactic longitude

A

l = CGX

angle between the galactic centre the galactic North Pole and the star

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4
Q

Galactic latitude

A

b = 90° - GX

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5
Q

the stars velocity due solely to the rotation of the Milky Way

A

v = ω x R

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6
Q

the suns velocity due solely to the rotation of the Milky Way

A

v_sun = ω_sun x R_sun

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7
Q

the position of the star

A

R = R_sun + ds

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8
Q

Stars motion with respect to the sun

A

v = v - v_sun

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9
Q

Relation between Oorts constants A and B

A

A - B = Omega 0

A - B = Vc/R

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10
Q

Circular velocity

A

Vc = (GM/R)^(1/2)

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11
Q

The number of galaxies per Mpc^3

A

N = ( L ∫ 0) Φ(L)

The galactic luminosity function = Φ(L)

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12
Q

Relation between Φ(L) and Φ(M)

A

Φ(M) = - Φ(L) dL/dM

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13
Q

Surface brightness

A

I(R) = F/Ω

where Ω = S/D^2

and F and Ω are both proportional to 1/d^2

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14
Q

Flux in terms of density

A

F = fsun ∫ pdz . S

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15
Q

Luminosity

A

L =2π (∞ ∫ 0) I(R)RdR

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16
Q

3-dimensional luminosity density

A

I(R) = (∞ ∫ -∞) j(r) dz

z^2 = r^2 - R^2

to find dz

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17
Q

Schechter function

A

Φs(L)dL on formula sheet

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18
Q

Redshift

A

z = v/c = ∆λ/λ

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19
Q

Time for an encounter to occur

A

tencounter = 1/πr^2vn

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20
Q

Gauss’s law

A

∇ . F = - 4πGp

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21
Q

Virial theorem

A

2<T> + <u> = 0</u></T>

T = 1/2Nmv^2

U = GM^2/R

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22
Q

Crossing time

A

Tcross = 2R/V

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23
Q

Fraction of spirals

A

f = ns/ntot

where ntot = ne + ns

e for elliptical

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24
Q

A(m)

A

= dN/dm = dN/dM

= (∞ ∫ 0) Φ(M)r^2dr

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25
Malmquist Bias
M0 - = σ^2 dlnA(m)/dm
26
Derive poisson’s equation
F = -∇Φ ∇.F = -4πGp substitute F in giving ∇Φ^2 = 4πGp
27
Derive oorts constants if vlos = ϴcosα - ϴ0sinl and μ = ϴsinα - ϴ0cosl
Assuming circular and planar motion replace ϴ = Ω/R Rcosα = R0sinl Rsinα = R0cosl - d Taylor expand to first order Ω = Ω0(R0) + d Ω0/dR|R0 (R-R0) Ω - Ω0(R0) = d Ω0/dR|R0 (R-R0) Ω = ϴ/R so replace d Ω0/dR|R0 (R-R0) = -dcosθ cos2θ= 2cos^2θ -1
28
Relaxation time
When Δv^2 = v^2
29
Strong encounters
rs < 2Gm/v^2
30
derive a weak encounters
when r0 > rs > 2Gm/v^2 Force on formula sheet Perpendicular component cos theta = b/r where r = b^2 + v^2t^2 F = M dv/dt Integrate 1/(a^2+s^2)^(3/2) = 2/a^2 giving Δv(perp) = 2Gm/bv
31
minimum for a weak encounter
bmin = 2Gm/v^2
32
Schechter function - total number of galaxies
ntot = Φ* Γ(alpha + 1)
33
Schechter function - total luminosity
Ltot = Φ* L*Γ(alpha + 2)
34
Cylindrical coordinate system in terms of Π, Θ and Z
<Π> = dR/dt = 0 = R dθ/dt = 0 <Θ> = dz/dt ≠ 0
35
LSR coordinate system
ΠLSR = 0 ΘLSR = Θ0 ZLSR = 0
36
Axisymmetric drift
< v > = -C < u^2 >
37
calculating peculiar velocities Δu, Δv and Δw
Δu = u - usun Δv = v - vsun Δw = w - wsun where usun = -<Δu>, vsun = -C - <Δv> and wsun = - <Δw>
38
how do we find
a least squares fit similiarly vsun is the intersect of the graph Δv versus σu^2, where C is the slope <Δv> = -C - vsun
39
Velocity of the LSR
Θ0 = R0(A-B)
40
Mean rotation period
t = 2π/Ω0 where Ω0 = Θ/R0
41
de Vaucoulers law
I(R) = IE exp[-7.67(R/RE)^1/4-1] where IE is the surface brightness at R = RE and RE is the radius at which the integrated luminosity is half the total
42
Derive the potential of a uniform sphere
poisson's equation and using spherical polar coordinates r^2 dΦ/dr = b Φ = -GM/r where b = GM
43
How do we calculate the potential of a flat disk?
through separation of variables J(R)Z(z).
44
Derive the star's energy for orbiting stars
d/dt(mv) + m.∇Φ(x) = 0 multiply by v where Φ(x) = -GM/x and dΦ/dt = v.∇Φ(x) d/dt[1/2mv^2] = mv(dot).v we get d/dt [1/2mv^2 + mΦ(x)] = 0 i.e. KE + PE = 0
45
escape speed
ve^2 = -2Φ(x) Φ(x) = -GM/x
46
speed of the Milky way at the distance of the Sun
v(R0) = Ω(R0)R0
47
rotational period of the Milky way at the distance of the sun
P(R0) = 2π/Ω(R0)
48
Derive the virial theorem if I = (N Σ i=1) miri.ri
differentiate with respect to time take the second derivative at equilibrium the moment of inertia is constant = - ∑i∑j Gmimj/2|rij|
49
Derive the relaxation time for a weak interaction given Δv(perp)= 2Gm/bv.
V = 2πbvt db N(collisions) = V x (N/Vsphere) < Δv(perp) >^2 = (bmax ∫ bmin) Δv(perp)^2 . N(collisions) Δv(perp)= 2Gm/bv bmax = R bmin = 1AU Trelax = Δv^2 = v^2
50
Elliptical galaxies - ellipticity.
N = 10(1-b/a) where the ellipticity ϵ = 1-b/a
51
Point-spread function P(d)
P(d) = 1/2πσ^2 exp[-d^2/2σ^2]
52
modified hubble law
Io = 2rojo
53
bulge fraction
B/T = LB/Ltot where Ltot = LD + LB
54
disk-to-bulge ratio
D/B = (B/T)^-1 Where T is the total
55
Peculiar velocities
u = Π - ΠLSR = Π v = Θ - ΘLSR = Θ-Θ0 w = Z - ZLSR = Z
56
Angular velocity curve
Ω(R) = Θ(R)/R
57
Derive the malmquist bias if A(m) = (∞ ∫ 0) Φ(M)r^2 dr Φ(M) = Φ0exp[-(M-M0)^2/2σ^2]
take the derivative with respect to M and divide through by A(m) rearranging gives as required
58
Derive the de Vaucouleurs surface brightness profile if m = a + bR^1/4 me = a + bRe^1/4 bRe^1/4/2.5 = 3.33
subtract the two relations m - me. use pogson's equation I(R) = Ie10^(-3.33[(R/R)^1/4 -1]) = Ie exp{-7.67[(R/Re)^1/4-1]}
59
Express the de Vaucoulers profile I(R) = Ie exp{-7.67[(R/Re)^1/4 -1]} in the form of the Sersic profile I(R) = I0 exp{-(R/𝛼)^1/n}
Take the exp{-7.67} out comparing the form we can see I0 = Ie exp{7.67} n = 4 and 𝛼 = Re/(7.67)^4
60
Intensity
I = F/θ^2
61
ϴ0
ϴ0 = ϴ(R0) where R0 is the galactocentric distance
62
Volume swept out by a star
V = πr^2vt