Stellar mass black holes

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Stellar mass black holes Now we know that massive stars make black holes Black hole mass: A few solar masses But how do we find such black holes? Gravity on other star? Light bending? Radiation?

Transcript of Stellar mass black holes

Stellar mass black holes• Now we know that massive stars make black holes

• Black hole mass: A few solar masses

• But how do we find such black holes?

Gravity on other star?

Light bending?

Radiation?

Most stars are “binaries”

• They have a stellar companion

• They orbit each other following Kepler’s laws

• Most massive stars should have a companion

• Massive stars evolve into black holes

Some hold on to their companions when they make black holes

⇒ Some black holes have stellar companions

Accretion• When a black hole comes close

enough:

It can syphon off matter from the companion star!

This matter must ultimately fall into the black hole

This process is called accretion

• This is how black holes grow

• This is how we find and study most black holes

Binary accretion• How can matter flow from one

star to another?

• Both stars orbit each other

Now we have two figure skaters...

2x gravity + centrifugal barrier

The “Roche potential”• Recall the effective potential

• The same for two masses:

Rotation + gravity

Curves: Lines of equal energy

“Free” to move along these lines

• Four classes of lines

Around both masses

Around one

Around none

The “Roche lobes” (thick black lines)

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RS unstable stable

Roche lobe overflow• Surfaces enclosing one mass:

“Roche Lobes”

Inside: objects are “bound”

At the solid black line: Can move freely from one object to other

In the middle: unstable point

• Two options:

Companion star smaller

Nothing happens

Companion star bigger

Matter will flow...

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Accretion disks• Recall the skater...:

Matter cannot fall straight in

It must lose angular momentum

• Forces:

Gravity (pulls in and down)

Centrifugal (pushes out)

Accretion disks• Recall the skater...:

Matter cannot fall straight in

It must lose angular momentum

• Forces:

Gravity (pulls in and down)

Centrifugal (pushes out)

⇒ Matter forms rotating disk

Matter slowly spirals in (like water going down a drain)

It speeds up (just like going down a slide)

Friction heats it up and it begins to shine brightly

Accretion disks

Accretion power: gravity

en

ergy

• Einstein: E=mc2

Gasoline powered (chemical) car: 45 mpg

Efficiency: 1 gram of energy for every 2000 tons of fuel

Efficiency (chemistry)

• Einstein: E=mc2

Nuclear (fission) powered car: 200 million mpg

Efficiency: 1 gram of energy for every 2 kilograms of fuel

Efficiency (nuclear power)

• Einstein: E=mc2

Nuclear (fusion) powered car: 4 billion mpg

Efficiency: 1 gram of energy for every 100 grams of fuel

Efficiency (nuclear power)

• Einstein: E=mc2

Black hole (accretion) powered car: 45 billion mpg

Efficiency: 1 gram of energy for every 10 grams of fuel

Efficiency (gravity)

Artist’s rendition

Gra

vita

tiona

l ene

rgy

Gravity power• Most of the energy release:

Close to the object:

• half the distance = twice the energy

The smaller the object, the more energy

• If you drop an object onto

sun : white dwarf : black hole

• you get energy return of

1 : 1000 : 500,000

Distance from object

Accretion disks• What transports the angular

momentum?

Friction (viscosity)

• Friction in astronomy always small

Matter must move in slowly

⇒ Almost perfect circular orbits

• Particles on Kepler orbits!

Inner orbits move faster

Inner orbits: more energy

⇒ Inner disk is hotter

Accretion disks• What transports the angular

momentum?

Friction (viscosity)

• Friction in astronomy always small

Matter must move in slowly

⇒ Almost perfect circular orbits

• Particles on Kepler orbits!

Inner orbits move faster

Inner orbits: more energy

⇒ Inner disk is hotter

side view

20 million degrees

X-rays!

X-ray binaries

X-ray binaries• Accretion onto neutron stars

and black holes:

Bright X-ray sources

First detected X-ray source: Scorpius X-1 (neutron star)

• How bright?

100,000 x sun

Easy to see in other galaxies

A binary in our Galaxy can destroy X-ray instruments

Messier 83, 15 million lightyears away

• Accretion is violent:

A planet would be shredded in seconds

Magnetic eruptions constantly dissipate energy

⇒ Flares, bursts, flashes...

X-Ray Binaries

How do we know magnetic things flare?

The sun in X-rays: Magnetic dissipation

X-Ray Binaries• Accretion is violent:

A planet would be shredded in seconds

Magnetic eruptions constantly dissipate energy

⇒ Flares, bursts, flashes...

Time (20 seconds)

Inte

nsity

The Eddington limit

The Eddington limit• So: 10% efficiency

• That means:

The more you accrete, the more you shine

• Is there a limit?

The Eddington limit• Where does all the radiation go?

Outward

It must go through incoming gas

⇒ Radiation pressure

The Eddington limit• Where does all the radiation go?

Outward

It must go through incoming gas

⇒ Radiation pressure

• When radiation pressure outweighs gravity:

No more accretion

No more radiation

⇒ Maximum power:

⇒ 500,000 x Psun x M/Msun