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Lecture 4 Turbulence and Magnetic Fields in Molecular Clouds Herschel Image of the Rosette Cloud
Transcript
Page 1: Lecture 4 Turbulence and Magnetic Fields in Molecular Cloudsastro1.physics.utoledo.edu/~megeath/ph6820/lecture4_ph6820.pdf · J = 6 pc M J = 450 Msun (cloud size) For n(H 2) = 100

Lecture 4Turbulence and Magnetic

Fields in Molecular Clouds

Herschel Image of the Rosette Cloud

Page 2: Lecture 4 Turbulence and Magnetic Fields in Molecular Cloudsastro1.physics.utoledo.edu/~megeath/ph6820/lecture4_ph6820.pdf · J = 6 pc M J = 450 Msun (cloud size) For n(H 2) = 100

Molecular Cloud PropertiesComposition: H2, He, dust (1% mass), CO (10-4 by number), and many other molecules with low abundances.

Sizes: 10-100 pc

Masses: 10 to 106 Msun. Most of the molecular gas mass in galaxies is found in the more massive clouds.

Average Density: 100 cm-3

Gas Temperature: 10-30 K

Page 3: Lecture 4 Turbulence and Magnetic Fields in Molecular Cloudsastro1.physics.utoledo.edu/~megeath/ph6820/lecture4_ph6820.pdf · J = 6 pc M J = 450 Msun (cloud size) For n(H 2) = 100

Review: Properties of Molecular Clouds

3Heyer et al. 2009

Virial

BoundNote: alpha may be underestimated if clouds are centrally condensed

Page 4: Lecture 4 Turbulence and Magnetic Fields in Molecular Cloudsastro1.physics.utoledo.edu/~megeath/ph6820/lecture4_ph6820.pdf · J = 6 pc M J = 450 Msun (cloud size) For n(H 2) = 100

4

The Stability of Clouds: Jeans Instability

Page 5: Lecture 4 Turbulence and Magnetic Fields in Molecular Cloudsastro1.physics.utoledo.edu/~megeath/ph6820/lecture4_ph6820.pdf · J = 6 pc M J = 450 Msun (cloud size) For n(H 2) = 100

5

Are Clouds Stable to Fragmentation?For n(H2) = 40 cm-3 λJ = 6 pc MJ = 450 Msun (cloud size)

For n(H2) = 100 cm-3 λJ = 4. pc MJ = 350 Msun (cloud size)

For n(H2) = 1000 cm-3 λJ = 1.2 pc MJ = 100 Msun (clump size)

From clouds in the inner galaxy from Heyer et al. 2009

Cloud masses and lengths exceed Jeans length masses.

Page 6: Lecture 4 Turbulence and Magnetic Fields in Molecular Cloudsastro1.physics.utoledo.edu/~megeath/ph6820/lecture4_ph6820.pdf · J = 6 pc M J = 450 Msun (cloud size) For n(H 2) = 100

6

Typical cloud efficiencies are a few percent for molecular clouds

From Evans et al. 2009

Star Formation Efficiency

Page 7: Lecture 4 Turbulence and Magnetic Fields in Molecular Cloudsastro1.physics.utoledo.edu/~megeath/ph6820/lecture4_ph6820.pdf · J = 6 pc M J = 450 Msun (cloud size) For n(H 2) = 100

7

Typical cloud efficiencies are a few percent for molecular clouds

From Evans et al. 2009

Star Formation Efficiency

Page 8: Lecture 4 Turbulence and Magnetic Fields in Molecular Cloudsastro1.physics.utoledo.edu/~megeath/ph6820/lecture4_ph6820.pdf · J = 6 pc M J = 450 Msun (cloud size) For n(H 2) = 100

Lifetimes of Nearby Clouds

Page 9: Lecture 4 Turbulence and Magnetic Fields in Molecular Cloudsastro1.physics.utoledo.edu/~megeath/ph6820/lecture4_ph6820.pdf · J = 6 pc M J = 450 Msun (cloud size) For n(H 2) = 100

Converging Flows

H2

HI fl

ow (f

rom

bub

ble

as e

xam

ple)

Heitsch et al. In press

HI fl

ow (f

rom

bub

ble

as e

xam

ple)

Page 10: Lecture 4 Turbulence and Magnetic Fields in Molecular Cloudsastro1.physics.utoledo.edu/~megeath/ph6820/lecture4_ph6820.pdf · J = 6 pc M J = 450 Msun (cloud size) For n(H 2) = 100

The Destruction of Molecular Clouds

M16

Page 11: Lecture 4 Turbulence and Magnetic Fields in Molecular Cloudsastro1.physics.utoledo.edu/~megeath/ph6820/lecture4_ph6820.pdf · J = 6 pc M J = 450 Msun (cloud size) For n(H 2) = 100

What Drives the Colliding Flows?

11N44 Superbubble in LMC

Page 12: Lecture 4 Turbulence and Magnetic Fields in Molecular Cloudsastro1.physics.utoledo.edu/~megeath/ph6820/lecture4_ph6820.pdf · J = 6 pc M J = 450 Msun (cloud size) For n(H 2) = 100

The Virial Theorem for Molecular Clouds

12

Page 13: Lecture 4 Turbulence and Magnetic Fields in Molecular Cloudsastro1.physics.utoledo.edu/~megeath/ph6820/lecture4_ph6820.pdf · J = 6 pc M J = 450 Msun (cloud size) For n(H 2) = 100

13

Virial Theorem with External Pressure

Page 14: Lecture 4 Turbulence and Magnetic Fields in Molecular Cloudsastro1.physics.utoledo.edu/~megeath/ph6820/lecture4_ph6820.pdf · J = 6 pc M J = 450 Msun (cloud size) For n(H 2) = 100

Comparing the internal and external pressure of molecular clouds

• A self gravitating gas with AV > 2 has an internal pressure of P/k > 2 x 104 cm-3 K.

• P/k = 100 cm-3 σ2 μ mH = 3 x 104 cm-3 K (σ = 1 km s-1)

• Typical external ISM gas pressure is P/k = 2 x 104 cm-3 K

• Molecular clouds with AV > 2 and n > 100 cm-3 are not pressure confined. 14

Page 15: Lecture 4 Turbulence and Magnetic Fields in Molecular Cloudsastro1.physics.utoledo.edu/~megeath/ph6820/lecture4_ph6820.pdf · J = 6 pc M J = 450 Msun (cloud size) For n(H 2) = 100

15

Could a thermally supported cloud be stable?

Page 16: Lecture 4 Turbulence and Magnetic Fields in Molecular Cloudsastro1.physics.utoledo.edu/~megeath/ph6820/lecture4_ph6820.pdf · J = 6 pc M J = 450 Msun (cloud size) For n(H 2) = 100

Could a thermally supported cloud be stable?

16

Page 17: Lecture 4 Turbulence and Magnetic Fields in Molecular Cloudsastro1.physics.utoledo.edu/~megeath/ph6820/lecture4_ph6820.pdf · J = 6 pc M J = 450 Msun (cloud size) For n(H 2) = 100

Could a thermally supported cloud be stable?

17

M = 104 MsunTK = 20 K (cs = 0.25 km s-1)=> Rcrit = 200 pc

But most clouds are much smaller. Also, considering only thermal motions α = |Ω/K| ~6 - thus not virialized

Furthermore Jeans criterion means that clouds are unstable to fragmentation

Page 18: Lecture 4 Turbulence and Magnetic Fields in Molecular Cloudsastro1.physics.utoledo.edu/~megeath/ph6820/lecture4_ph6820.pdf · J = 6 pc M J = 450 Msun (cloud size) For n(H 2) = 100

Timescales• Star formation lifetime < 5 Myr

18

t = length/σ

Star formation timescale comparable to cloud free-fall time and larger than crossing time.

Star formation time > cloud free-fall time. This suggest some sort of support.

Page 19: Lecture 4 Turbulence and Magnetic Fields in Molecular Cloudsastro1.physics.utoledo.edu/~megeath/ph6820/lecture4_ph6820.pdf · J = 6 pc M J = 450 Msun (cloud size) For n(H 2) = 100

19

Could Magnetic Fields Support Clouds?

Page 20: Lecture 4 Turbulence and Magnetic Fields in Molecular Cloudsastro1.physics.utoledo.edu/~megeath/ph6820/lecture4_ph6820.pdf · J = 6 pc M J = 450 Msun (cloud size) For n(H 2) = 100

Magnetic Fields in Galaxies

Page 21: Lecture 4 Turbulence and Magnetic Fields in Molecular Cloudsastro1.physics.utoledo.edu/~megeath/ph6820/lecture4_ph6820.pdf · J = 6 pc M J = 450 Msun (cloud size) For n(H 2) = 100

Magnetic field Orientation in

the Orion Molecular

Cloud

Polarization of emission from grains at 850 microns. Polarization perpendicular to B

Matthews 2001 ApJ 562, 400.

Page 22: Lecture 4 Turbulence and Magnetic Fields in Molecular Cloudsastro1.physics.utoledo.edu/~megeath/ph6820/lecture4_ph6820.pdf · J = 6 pc M J = 450 Msun (cloud size) For n(H 2) = 100

Could Magnetic Fields Support Clouds?

22

Page 23: Lecture 4 Turbulence and Magnetic Fields in Molecular Cloudsastro1.physics.utoledo.edu/~megeath/ph6820/lecture4_ph6820.pdf · J = 6 pc M J = 450 Msun (cloud size) For n(H 2) = 100

Could Magnetic Fields Support Clouds?

23

Page 24: Lecture 4 Turbulence and Magnetic Fields in Molecular Cloudsastro1.physics.utoledo.edu/~megeath/ph6820/lecture4_ph6820.pdf · J = 6 pc M J = 450 Msun (cloud size) For n(H 2) = 100

What is the mass to flux ratio?

24

B can be measured by the Zeeman effect to OH or HI

N(H2) can be measured my molecular line or extinction measurements

Page 25: Lecture 4 Turbulence and Magnetic Fields in Molecular Cloudsastro1.physics.utoledo.edu/~megeath/ph6820/lecture4_ph6820.pdf · J = 6 pc M J = 450 Msun (cloud size) For n(H 2) = 100

The data: are molecular clouds supercritical or subcritical?

25

Diffuse ISMSub-Critical

Molecular Clouds: Critical

Critical

Page 26: Lecture 4 Turbulence and Magnetic Fields in Molecular Cloudsastro1.physics.utoledo.edu/~megeath/ph6820/lecture4_ph6820.pdf · J = 6 pc M J = 450 Msun (cloud size) For n(H 2) = 100

The data: are molecular clouds supercritical or subcritical?

• Current consensus is that magnetic fields do not provide support against collapse.

• This makes some sense, if magnetic fields dominated, then the clouds would expand.

• However, there are significant uncertainties in the data.

• However, magnetic fields may be strong enough to play some role in cloud evolution, this is an area of intense research.

26

Page 27: Lecture 4 Turbulence and Magnetic Fields in Molecular Cloudsastro1.physics.utoledo.edu/~megeath/ph6820/lecture4_ph6820.pdf · J = 6 pc M J = 450 Msun (cloud size) For n(H 2) = 100

Can Turbulence Stabilize Clouds?

27

Page 28: Lecture 4 Turbulence and Magnetic Fields in Molecular Cloudsastro1.physics.utoledo.edu/~megeath/ph6820/lecture4_ph6820.pdf · J = 6 pc M J = 450 Msun (cloud size) For n(H 2) = 100

Kinematics and Morphology of Orion Cloud

28

Page 29: Lecture 4 Turbulence and Magnetic Fields in Molecular Cloudsastro1.physics.utoledo.edu/~megeath/ph6820/lecture4_ph6820.pdf · J = 6 pc M J = 450 Msun (cloud size) For n(H 2) = 100

Turbulent Pressure

29

Page 30: Lecture 4 Turbulence and Magnetic Fields in Molecular Cloudsastro1.physics.utoledo.edu/~megeath/ph6820/lecture4_ph6820.pdf · J = 6 pc M J = 450 Msun (cloud size) For n(H 2) = 100

Supersonic Motions in Clouds

Sound speed in molecular clouds

cs = (kT/μmH)1/2

cs = 0.25 km s-1 for T = 20 K

Page 31: Lecture 4 Turbulence and Magnetic Fields in Molecular Cloudsastro1.physics.utoledo.edu/~megeath/ph6820/lecture4_ph6820.pdf · J = 6 pc M J = 450 Msun (cloud size) For n(H 2) = 100

Can Turbulence Stabilize Clouds?

• M = 104 Msunσ = 1km s-1

=> Rcrit = 12 pc• α = |Ω/K| ~1 (2 needed for virial)

• This looks good, but there could still Jeans fragmentation• Plus, turbulence may aid fragmentation (turbulent

fragmenation)

31

Page 32: Lecture 4 Turbulence and Magnetic Fields in Molecular Cloudsastro1.physics.utoledo.edu/~megeath/ph6820/lecture4_ph6820.pdf · J = 6 pc M J = 450 Msun (cloud size) For n(H 2) = 100

Shock Waves

• Occur when two parcels of gas collide at supersonic velocities.

• Collision results in the compression of the gas. • In sub-sonic case, compression would result in

pressure (sound) waves.• Since motion is faster than speed of sound, a

dense layer of shock gas is produced.• If gas cools rapidly, then shock will dissipate

energy. 32

Page 33: Lecture 4 Turbulence and Magnetic Fields in Molecular Cloudsastro1.physics.utoledo.edu/~megeath/ph6820/lecture4_ph6820.pdf · J = 6 pc M J = 450 Msun (cloud size) For n(H 2) = 100

Shock Waves

33

Page 34: Lecture 4 Turbulence and Magnetic Fields in Molecular Cloudsastro1.physics.utoledo.edu/~megeath/ph6820/lecture4_ph6820.pdf · J = 6 pc M J = 450 Msun (cloud size) For n(H 2) = 100

Driven Turbulence

in a Periodic

Box

Frrom Paolo Padon’s website: http://cass246.ucsd.edu/~ppadoan/new_website/astrophysical.php

Page 35: Lecture 4 Turbulence and Magnetic Fields in Molecular Cloudsastro1.physics.utoledo.edu/~megeath/ph6820/lecture4_ph6820.pdf · J = 6 pc M J = 450 Msun (cloud size) For n(H 2) = 100

Self-gravitating

turbulent gas with periodic

boundary condition

Density projection (column density?)

Paolo Padoan’s website: http://cass246.ucsd.edu/~ppadoan/new_website/astrophysical.php

Page 36: Lecture 4 Turbulence and Magnetic Fields in Molecular Cloudsastro1.physics.utoledo.edu/~megeath/ph6820/lecture4_ph6820.pdf · J = 6 pc M J = 450 Msun (cloud size) For n(H 2) = 100

Cluster Formation in a Turbulent Cloud

36

Page 37: Lecture 4 Turbulence and Magnetic Fields in Molecular Cloudsastro1.physics.utoledo.edu/~megeath/ph6820/lecture4_ph6820.pdf · J = 6 pc M J = 450 Msun (cloud size) For n(H 2) = 100

Can Turbulence Stabilize Clouds?

• The problem is that turbulence can decay rapidly.

• The decay timescale is a fraction of a crossing time.

37

Page 38: Lecture 4 Turbulence and Magnetic Fields in Molecular Cloudsastro1.physics.utoledo.edu/~megeath/ph6820/lecture4_ph6820.pdf · J = 6 pc M J = 450 Msun (cloud size) For n(H 2) = 100

Kinetic Energy Decay

323 2563

ZEUShydro

weakMHD

SPHhydro

strongMHD

193703

ML,

Kle

ssen

, Bur

kert,

Sm

ith (1

998,

Phy

s. R

ev. L

ett.)

Page 39: Lecture 4 Turbulence and Magnetic Fields in Molecular Cloudsastro1.physics.utoledo.edu/~megeath/ph6820/lecture4_ph6820.pdf · J = 6 pc M J = 450 Msun (cloud size) For n(H 2) = 100

Nakamujra & Li 2007

Outflow Driven TurbulenceSimulation of a cluster forming clump within cloud. Outflows from stars in cloud eject gas, gas falls back on clump and stirs the turbulence.

Page 40: Lecture 4 Turbulence and Magnetic Fields in Molecular Cloudsastro1.physics.utoledo.edu/~megeath/ph6820/lecture4_ph6820.pdf · J = 6 pc M J = 450 Msun (cloud size) For n(H 2) = 100

Timescales• Star formation lifetime < 5 Myr

40

t = length/σ

Star formation timescale comparable to cloud free-fall time and larger than crossing time.

Star formation time > cloud free-fall time. This suggest some sort of support.

Page 41: Lecture 4 Turbulence and Magnetic Fields in Molecular Cloudsastro1.physics.utoledo.edu/~megeath/ph6820/lecture4_ph6820.pdf · J = 6 pc M J = 450 Msun (cloud size) For n(H 2) = 100

What is the role of turbulence?

41

• Decay of turbulence may happen, but perhaps decay on the order of a crossing time, which can be 10 Myr on the longest scale, is OK.

• Turbulence may delay collapse to more than one free fall time.

• Although turbulence may slow the collapse of the cloud, it will also enhance fragmentation and lead to the fragmentation of the gas into individual stars.

• Stars that are formed by turbulence can stir up gas (feedback), but will also destroy clouds

Page 42: Lecture 4 Turbulence and Magnetic Fields in Molecular Cloudsastro1.physics.utoledo.edu/~megeath/ph6820/lecture4_ph6820.pdf · J = 6 pc M J = 450 Msun (cloud size) For n(H 2) = 100

Summary1. Molecular clouds are confined by gravity and not external

pressure.

2. Thermally supported clouds are unstable

3. Molecular fields are unlikely to stabilize cloud

4. Turbulence may support clouds on large scales, but cause fragmentation on much smaller scales.


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