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Day 2, Topic 2: Self-gravitating hydrostatic gas spheres Lecture by: CP. Dullemond The formation of stars and planets |
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B68: a self-gravitating stable cloudBok Globule Relatively isolated, hence not many external disturbances Though not main mode of star formation, their isolation makes them good test-laboratories for theories! |
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Hydrostatic self-gravitating spheresSpherical symmetry Isothermal Molecular From here on the material is partially based on the book by Stahler & Palla “Formation of Stars” |
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Hydrostatic self-gravitating spheresSpherical coordinates: |
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Hydrostatic self-gravitating spheresSpherical coordinates: |
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Hydrostatic self-gravitating spheresNumerical solutions: |
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Hydrostatic self-gravitating spheresNumerical solutions: Exercise: write a small program to integrate these equations, for a given central density |
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Hydrostatic self-gravitating spheresNumerical solutions: |
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Hydrostatic self-gravitating spheresNumerical solutions: Plotted logarithmically (which we will usually do from now on) Bonnor-Ebert Sphere |
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Hydrostatic self-gravitating spheresDifferent starting ?o : a family of solutions Numerical solutions: |
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Hydrostatic self-gravitating spheresNumerical solutions: Singular isothermal sphere (limiting solution) |
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Hydrostatic self-gravitating spheresNumerical solutions: Boundary condition: Pressure at outer edge = pressure of GMC |
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Hydrostatic self-gravitating spheresNumerical solutions: One boundary condition too many! Another boundary condition: Mass of clump is given |
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Hydrostatic self-gravitating spheresSummary of BC problem: For inside-out integration the paramters are ?c and ro. However, the physical parameters are M and Po We need to reformulate the equations: Write everything dimensionless Consider the scaling symmetry of the solutions |
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Hydrostatic self-gravitating spheresAll solutions are scaled versions of each other! |
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Hydrostatic self-gravitating spheresA dimensionless, scale-free formulation: |
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Hydrostatic self-gravitating spheresA dimensionless, scale-free formulation: Lane-Emden equation |
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Hydrostatic self-gravitating spheresA dimensionless, scale-free formulation: Boundary conditions (both at ?=0): Numerically integrate inside-out |
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Hydrostatic self-gravitating spheresA dimensionless, scale-free formulation: A direct relation between ?o/?c and ?o |
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Hydrostatic self-gravitating spheresWe wish to find a recipe to find, for given M and Po, the following: ?c (central density of sphere) ro (outer radius of sphere) Hence: the full solution of the Bonnor-Ebert sphere Plan: Express M in a dimensionless mass ‘m’ Solve for ?c/?o (for given m) (since ?o follows from Po = ?ocs2 this gives us ?c) Solve for ?o (for given ?c/?o) (this gives us ro) |
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Hydrostatic self-gravitating spheres |
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Hydrostatic self-gravitating spheres |
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Hydrostatic self-gravitating spheresRecipe: Convert M in m (for given Po), find ?c/?o from figure, obtain ?c, use dimless solutions to find ro, make BE sphere Dimensionless mass: |
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Stability of BE spheresMany modes of instability One is if dPo/dro > 0 Run-away collapse, or Run-away growth, followed by collapse Dimensionless equivalent: dm/d(?c/?o) < 0 |
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Stability of BE spheres |
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Bonnor-Ebert massWays to cause BE sphere to collapse: Increase external pressure until MBE<M Load matter onto BE sphere until M>MBE |
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Bonnor-Ebert massNow plotting the x-axis linear (only up to ?c/?o =14.1) and divide y-axis through BE mass: Hydrostatic clouds with large ?c/?o must be very rare... |
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BE ‘Sphere’: Observations of B68Alves, Lada, Lada 2001 |
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Magnetic field support / ambipolar diffAs mentioned in previous chapter, magnetic fields can partly support cloud and prevent collapse. Slow ambipolar diffusion moves fields out of cloud, which could trigger collapse. Models by Lizano & Shu (1989) show this elegantly: Magnetic support only in x-y plane, so cloud is flattened. Dashed vertical line is field in beginning, solid: after some time. Field moves inward geometrically, but outward w.r.t. the matter. |
«Day 2, Topic 2: Self-gravitating hydrostatic gas spheres Lecture by: C.P. Dullemond» |
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