accretion in binaries ii

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Accretion in Binaries II • Classes of X-ray binaries – Low-mass (BH and NS) – High-mass (BH and NS) – X-ray pulsars (NS) – Be/X-ray binaries (NS) • Distinguishing NS versus BH binaries

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Accretion in Binaries II. Classes of X-ray binaries Low-mass (BH and NS) High-mass (BH and NS) X-ray pulsars (NS) Be/X-ray binaries (NS) Distinguishing NS versus BH binaries. X-Ray Binaries. Low mass: companion star mass less than one solar mass - PowerPoint PPT Presentation

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Page 1: Accretion in Binaries II

Accretion in Binaries II

• Classes of X-ray binaries– Low-mass (BH and NS)– High-mass (BH and NS)– X-ray pulsars (NS)– Be/X-ray binaries (NS)

• Distinguishing NS versus BH binaries

Page 2: Accretion in Binaries II

X-Ray Binaries

• Low mass: companion star mass less than one solar mass

• High mass: companion star mass greater than one solar mass.

Page 3: Accretion in Binaries II

bow shockmatter collects in wake

racc

Wind Fed Accretion

Page 4: Accretion in Binaries II

Wind Fed Accretion

Matter in wind will accrete if its speed is less than the escape speed from the compact object at the radius of closest approach

Vw = wind velocity

Vx = velocity of compact object

Rc = capture radius

22

2

WX

Xc VV

GMR

Page 5: Accretion in Binaries II

Luminosity

Xwworb

w

orb

accw

vvifvD

GMcmcmL

D

rmm

,2

4

4

4

222

2

If a neutron star binary has the followingparameters, Dorb=1012 cm, vw= 1000 km/s,

)(1044

1 242

42

cmcmv

c

D

RL ww

worb

s

Page 6: Accretion in Binaries II

Accreting Pulsars

High mass X-ray binary

Page 7: Accretion in Binaries II

Accretion in magnetic field

Page 8: Accretion in Binaries II

Magnetosphere boundary

Assuming spherical accretion and a dipole field with the dipole moment = BSRS

3, where RS and BS are the radius of the star and the field strength at the surface.

Magnetopheric boundary, rM, is where the magnetic pressure balances the ram pressure of accreted matter

22

8vp

Bp rammag

7/4

330

7/17/2

168

cmG10g/s10 cm101.5

M

MmrM

Page 9: Accretion in Binaries II

Accretion Torque

7/6

2

Find

2 and Note

staron Torque

transportmomentumAngular

PLP

P

PPr

mGML

rvmI

rvm

M

m

Page 10: Accretion in Binaries II

Accretion Torque

Page 11: Accretion in Binaries II

Pulse Period Variations

Page 12: Accretion in Binaries II

What happens if the spin rate of the pulsar is faster than Keplerian rotation rate at the magnetospheric boundary?

Corotation radius lies outside magnetopheric boundary

Page 13: Accretion in Binaries II

Equilibrium Period

The accreted matter ceases to transfer angular momentumto the neutron star when

For a maximum (Eddington) luminosity and typical neutron star mass and radius, we have

7/6

9min

G10002.0

B

s

P

7/6

14/312

2/1

2/13

8)(

22

)(

SM

eq

MK

BmGM

R

GMGM

rP

r

Page 14: Accretion in Binaries II

Emission Geometry

Accreted plasma

Shock front

Settling matterHot spot

Page 15: Accretion in Binaries II

Pulse Profiles

Page 16: Accretion in Binaries II

Landau Levels

Quantization of energy due to magnetic field:

Landau levels

where is the momentum of the electron parallel to the field,n is the quantum number, and Bcrit is the critical field,

||p

Ghe

cmB ecrit

1332

104.4

For B << Bcrit, the spacing between adjacent levels is

G

BkeVB

cm

ehEEE

enncyc 121 10

6.11

Page 17: Accretion in Binaries II

Cyclotron Lines

Page 18: Accretion in Binaries II

X-Ray Pulsar Cen X-3

Pulses are modulated at orbital period of 2.09 days

Page 19: Accretion in Binaries II

Distinguishing BH vs NS

G

KP

MM

iMfX

X

2)(

sin 300

20

33

0

XMf 0Mass function

Page 20: Accretion in Binaries II

Compact object masses