Changes between Version 32 and Version 33 of GravoTurbulence
- Timestamp:
- 12/15/11 16:01:06 (13 years ago)
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GravoTurbulence
v32 v33 42 42 So i modified the mean density to be 10, set [[latex($\alpha=-2$)]] so [[latex($\beta-1$)]] and strengthened the perturbation. 43 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 44 60 === II === 45 61 || II || … … 50 66 51 67 68 69 70 71 72 73 74 75 76 77 78 79 80 81 82 83 52 84 In all of these, there was initial pressure equilibrium (so different temperatues), although I was using a gamma=1.001 which assumes an isothermal gas. Consider what happens when a gas at a density of 1 and a temperature of 100 K mixes with a gas at a density of 100 and a temperature of 1 K. 53 85 … … 82 114 83 115 84 116 Unless the dense blobs are gravitationally confined. But how to go from a power spectra of density fluctuations to a mass-size relation? We have [[latex($\hat{\rho}(\mathbf{k}) \propto \exp^{A|k|^{\beta}}$)]]? If [[latex($k << \lambda_k = c_s\sqrt{\frac{\pi}{G}} \rho^{-1/2}$)]] then the fluctuations should be jeans unstable - but \rho = } 85 117 86 118