virial theorem stellar structurestellar structure of virial theorem 2e ke e grav 0 e tot e ke e grav...
TRANSCRIPT
Star produces energy via nuclear fusion
mass: 2×1030 kg
Sun:our nearest star
radius: 7×105 km(109×Earth radius)( )
N l f i f H d 6 1×1011 k dNuclear fusion of Hydrogen: 6.1×1011 kg per second 3.85×1026J / seccf. a nuclear power plant produce 109 J / sec
Stellar Structure静⽔圧平衡 (せいすいあつへいこう、hydrostatic equilibrium)
重⼒による収縮 と 圧⼒勾配による膨張が釣り合った状態Gravity balances with Pressure Gradient
What is pressure? L
# A particle collides with a wall perpendicular to x-axis.It gives momentum (運動量) to the wall
N particles
2 ( 2 )p(px,py,pz)
# A particle collides with the wall per unit time v(vx,vy,vz)
2px (=2mvx)
x# A particle gives momentum to the wall per unit time
vx/(2L) times
# Momentum given to a wall per unit time per unit area
2px ×vx/(2L) = px vx /L
g p p=Force given to a wall per unit area=pressure Total kinetic energy
of gas particles in a box
VEmvnvpn
LLvpNP KExx
32
21
32
311 2
2
“p” is momentum 運動量“P” is pressure
number density
Pressure Gradient
Diff ( di t) f t d + Positive = outward directionDifference (gradient) of pressure at r and r+r
ArdrdPAr
drdPrPrPArrPrP
)()()()(
Positive outward direction
drdr
rRr
rR
M=(r)rA
PA (P+P)A
M (r)rAArea A
Density and temperature is higher at inner radii 0dPDensity and temperature is higher at inner radii 0dr
Force by pressure gradient … positive = outward direction
Particle A pulls particle B by gravitational force
Gravity
mA mBr
Particle A pulls particle B by gravitational force
mGm BA2r
Gravitational energy of particle BmGm BAgy p
r
r
2
density
rRGas mass inside radius r
It gives gravity to■
rdrrrm 2
0
4)()(
M=(r)rAIt gives gravity to ■
])([)()( ArrrGmMrGm ])([22 Arr
rM
r
Balance between gravity and pressure gradient
0))(()( ArdPArrrGm
Gravity balances with Pressure Gradient
0))((2 Ardr
Arrr
dPrrGm )()( drd
rGm
2
)()(
rrR
r
PA (P+P)A
M=(r)rAArea A
Gravity: inwardsPressure gradient: outwards
Virial Theorem and Hydrostatic Equilibrium
2
)()(r
rrGmdrdP
Hydrostatic Equilibrium:
Multiply by 4 r3 and integrate from r = 0 to r=R
RR
drrrGmddP 23 4)()(4
=dm rdm dr
rdr
drr
00
3 )()(4
M
dm
Right term = M
gravEdmr
rGm
0
)(
Left term= drrdrrrP
drrrPrrPR
R
RR
20
2
23 44)(
304)(3]4)([
Left term= drrdrr
drrrPrrP R
0
0
200 4
4304)(3]4)([
= - 3<P>VE1 0
VE
P grav
31
weighted meanMean pressure weighted by volume
Virial Theorem and Hydrostatic Equilibrium
VE
P grav
31
Mean pressure in a starV3
VEP KE
32
SubstituteV
EV
E KEgrav
32
31
V3 VV 33
Virial Theorem
02 gravKE EE1
gravKEgravKETOT EEEEE21
Application of Virial Theorem
02 gravKE EE
gravKEgravKETOT EEEEE21
・ETOT < 0 …bound
2
・When energy is lost (ETOT decreased), temperature rises (EKE increased)
Photon is emitted from stellar
example:Kelvin-Helmholtz Contraction
Photon is emitted from stellar surface Energy is lost
ETOT & E decrease
Gas contractsto get hotter
ETOT & Egrav decrease EKE increase
Contraction stopswhen the temperature and density get highenough for nuclear fusion
Starルツシ プルング ラ セル図
brヘルツシュプルング-ラッセル図Surface temperature vs brightness 重い
right
巨星惑星状星雲
Most stars are plotted along a lineMain sequence...Main sequencenuclear fusion of Hydrogen to Helium
Sun
Massive MS stars are rareformation rate is low
軽いspectrum type mass life time [yr]
B 20 107
... formation rate is lowshort lifetime
faint
high← temperature → low
B 20 107
A 3 5×108
G 1 1010
spectrum typeK 0.6 1011