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The Physics of the ICM core: Conduction, the HBI, and cold filaments The Physics of the ICM core: Conduction, the HBI, and cold filaments

The Physics of the ICM core: Conduction, the HBI, and cold filaments - PowerPoint Presentation

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The Physics of the ICM core: Conduction, the HBI, and cold filaments - PPT Presentation

Chris Reynolds UMd with Mark Avara UMd Steve Balbus Oxford Tamara Bogdanovic Georgia Tech Matt Kunz Princeton 29th August 2012 Michigan workshop Outline Motivation why study conduction in ICM cores ID: 630863

29th august michigan 2012 august 29th 2012 michigan workshop agn filaments amp hbi field heating core icm conduction thermal

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Slide1

The Physics of the ICM core: Conduction, the HBI, and cold filaments

Chris Reynolds (UMd)with…Mark Avara (UMd)Steve Balbus (Oxford)Tamara Bogdanovic (Georgia Tech)Matt Kunz (Princeton)

29th August 2012

Michigan workshopSlide2

Outline

Motivation: why study conduction in ICM cores?Non-linear behaviour of the HBI(β, resolution) parameter space surveyHBI ≠ insulation of conductive heat fluxCold filaments in clustersSubtle nature of local thermal instabilityFilament condensation in Braginskii-MHD modelsAGN heating and the isotropy problem29th August 2012Michigan workshopSlide3

29th August 2012

Michigan workshopPerseus cluster (1Ms/Chandra)Fabian et al. (2011)3Gyr cooling radiusSlide4

Is all “just” AGN feedback, isn’t it?

Maybe but…Direct evidence for AGN heating is still elusive!Clearly lots of ICM-AGN interaction (cavities, ripples), but the heating mechanism remains elusive! Fail to see strong shocks!Effervescent heating (Roychowdhury+04), dissipation of sound waves (Fabian+05) or turbulence (Ruszkowski+10), CR heating… The isotropy problemThe obvious AGN energy output is in form of narrow jetsHow do jets heat the core isotropically? (Vernaleo

& CSR 2006)The multi-scale feedback problem

Cooling core ~100kpc, but accretion radius <10pcHow is such a tight feedback-loop maintained?

Still worth keeping an open mind about alternatives…

29th August 2012

Michigan workshopSlide5

(

azimuthal) (radial)(Outskirts)(Core)29th August 2012Michigan workshop>0

<0

Balbus & Reynolds (2010)Slide6

Can thermal conduction offset cooling throughout (at least some of) the ICM core?

29th August 2012Michigan workshopProblem: HBI = insulation

But is this true?? Slide7

29th August 2012

Michigan workshopHotColdBuffer (isotropic κ)

Buffer (isotropic κ

)

0.1H

Resolution N×N

Active region

(anisotropic

κ

)

2-d

Uniform gravity

Uniform

κ

No

radiative

cooling

Initially…

Linear temperature profile

Vertical uniform B-field

Examine

behaviour

as a function of numerical resolution and initial magnetic field

(

Avara

et al.)Slide8

29th August 2012

Michigan workshopSlide9

29th August 2012

Michigan workshopIncreasing resolutionIncreasing magnetic field strength

STABLE

HBI SHUTS OFF CONDUCTION

HEAT FLUX PERSISTS DESPITE HBI ACTIVITYSlide10

29th August 2012

Michigan workshopSlide11

29th August 2012

Michigan workshopPower-law spectrum of fluctuations rather than single mode…Slide12

29th August 2012

Michigan workshopFilaments are all HBI stable… they result from the competing need to satisfy magnetic flux conservation in the presence of an instability that actively re-orients vertical field. Slide13

29th August 2012

Michigan workshopSlide14

29th August 2012

Michigan workshopBogdanovic, Reynolds, Balbus & Parrish (2009)also see Parrish et al. (2009), Ruszkowski & Oh (2009, 2010)Temperature

Radial conductive heat fluxSlide15

Cold filaments, AGN fueling and the isotropy problem

29th August 2012Michigan workshopSlide16

29th August 2012

Michigan workshop7th April 2009IAS

Fabian et al. (2008)Slide17

29th August 2012

Michigan workshopSlide18

29th August 2012

Michigan workshopMcDonald et al. (2010)Also Voit et al. (2008)Slide19

29th August 2012

Michigan workshopKunz,Bogdanovic, Reynolds & Stone (2012) Slide20

29th August 2012

Michigan workshopCourtesy M.KunzSlide21

29th August 2012

Michigan workshopSlide22

Subtleties of local thermal instability

Classical Field result (no gravity):Buoyancy effects stabilize local thermal instability! If we have Lnet=L(ρ,P,T) then gas is locally thermally stable if atmosphere is convectively stable! (Balbus & Soker 1989)Why then do we see filaments collapsing?Significant heating via conduction, giving Lnet an explicit spatial dependenceDue to viscosity, atmosphere can be globally stabilized long enough for the local instability to work!

(Kunz et al. 2012)

Alternative… include a “bulk heating” term from the AGN that is a function of position (Sharma et al. 2012)

29th August 2012

Michigan workshopSlide23

29th August 2012

Michigan workshopSlide24

Conclusions

Reason to challenge HBI=insulation assertionLocal results depend upon initial field strengthGlobal results may be strongly resolution limitedCase that AGN heating dominates ICM core is still not solid!Cold filaments & AGN feedbackBraginskii viscosity promotes formation of cold filaments via local thermal instabilityHypothesis : AGN fed by filaments, jets periodically realigned, feedback isotropized over few cooling times. 29th August 2012Michigan workshop