Sue Ann Heatherly edited results_table.md  almost 10 years ago

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### Connections to Littlewood’s Conjecture  We show the energy radiated in the convective region to be proportional  to the mass in the radiative layer between the stellar surface and the  upper boundary of the convective zone, as shown in the following table and in Figure \ref{fig:fig1}:  |**Phase** | **Time** | **M\(_ 1\)** | **M\(_ 2\)** | **\(\Delta M\)** | **P** | **\(v_{\rm rot,1}\)** | **\(v_{\rm rot,2}\)** |   |:------------------|:----------|-------------|-------------|----------------|-------|---------------------|---------------------|  |1 ZAMS | 0 | 16 | 15 | – | 5.0 | 230 | 230 |   |2 Case B | 9.89 | 15.92 | 14.94 | 0.14 | 5.1 | 96 | 85 |   |3 ECCB | 11.30 | 3.71 | 20.86 | 6.44 | 42.7 | 40 | 767 |   |4 ECHB | 18.10 | – | 16.76 | – | – | – | 202 |   |5 ICB | 18.56 | – | 12.85 | – | – | – | 191 |   |6 ECCB | 18.56 | – | 12.83 | – | – | – | 258 | Galaxies  We see a different result when imaging galaxies. As seen in the figure below with M123, longer exposure times result in images with greater clarity.