Table 2.

Summary of results for all runs. All quantities reported here are averaged for |$t\gt 75$| Myr and |$z=L_z$|⁠. Column 2 – the mass loading factor (⁠|$\eta _M$|⁠). Column 3 – the burstiness parameter b (equation 8). Columns 4, 5, and 6 – the contribution to |$\eta _M$| from cool (⁠|$T\lt 2 \times 10^4$| K), warm unstable (⁠|$2 \times 10^4$| K |$\lt T\lt 10^6$| K), and hot (⁠|$T\gt 10^6$| K) gas, respectively. Columns 7 and 8 – the energy loading (⁠|$\eta _E$|⁠) and the metal loading (⁠|$\eta _Z$|⁠) factors. Column 9 – the average fraction of metals promptly lost to the wind rather than retained in the ISM |$\phi$| (equation 7).

Name|$\eta _M$|b|$\eta _M^{\rm cool}$||$\eta _M^{\rm warm}$||$\eta _M^{\rm hot}$||$\eta _E$||$\eta _Z$||$\phi$|
(1)(2)(3)(4)(5)(6)(7)(8)(9)
|$\Sigma$|13-Z1-H1502.11.00.820.311.00.641.00.97
|$\Sigma$|50-Z1-H1500.260.580.00.00.260.970.860.96
|$\Sigma$|2.5-Z1-H1502.32.00.201.690.170.0140.0930.052
|$\Sigma$|13-Z0.2-H1500.0402.7|$1.0\times 10^{-5}$|0.040|$1.4\times 10^{-4}$||$1.3\times 10^{-3}$||$6.0\times 10^{-3}$||$2.7\times 10^{-3}$|
|$\Sigma$|50-Z0.2-H1500.480.650.00.00.480.480.920.89
|$\Sigma$|2.5-Z0.2-H1501.62.10.0811.5|$5.5\times 10^{-3}$|0.0120.034|$4.5\times 10^{-3}$|
|$\Sigma$|2.5-Z1-H3000.282.8|$8.2\times 10^{-4}$|0.27|$7.9\times 10^{-3}$||$8.9\times 10^{-4}$|0.0170.014
|$\Sigma$|2.5-Z1-H1000|$3.2\times 10^{-3}$|3.0|$-2.7 \times 10^{-5}$||$3.3\times 10^{-3}$|0.0|$1.8\times 10^{-5}$||$5.7\times 10^{-4}$||$5.0\times 10^{-4}$|
|$\Sigma$|2.5-Z1-H15004.62.32.02.50.044|$2.9\times 10^{-3}$|0.270.18
|$\Sigma$|2.5-Z1-H20003.60.910.0191.71.80.390.620.56
Name|$\eta _M$|b|$\eta _M^{\rm cool}$||$\eta _M^{\rm warm}$||$\eta _M^{\rm hot}$||$\eta _E$||$\eta _Z$||$\phi$|
(1)(2)(3)(4)(5)(6)(7)(8)(9)
|$\Sigma$|13-Z1-H1502.11.00.820.311.00.641.00.97
|$\Sigma$|50-Z1-H1500.260.580.00.00.260.970.860.96
|$\Sigma$|2.5-Z1-H1502.32.00.201.690.170.0140.0930.052
|$\Sigma$|13-Z0.2-H1500.0402.7|$1.0\times 10^{-5}$|0.040|$1.4\times 10^{-4}$||$1.3\times 10^{-3}$||$6.0\times 10^{-3}$||$2.7\times 10^{-3}$|
|$\Sigma$|50-Z0.2-H1500.480.650.00.00.480.480.920.89
|$\Sigma$|2.5-Z0.2-H1501.62.10.0811.5|$5.5\times 10^{-3}$|0.0120.034|$4.5\times 10^{-3}$|
|$\Sigma$|2.5-Z1-H3000.282.8|$8.2\times 10^{-4}$|0.27|$7.9\times 10^{-3}$||$8.9\times 10^{-4}$|0.0170.014
|$\Sigma$|2.5-Z1-H1000|$3.2\times 10^{-3}$|3.0|$-2.7 \times 10^{-5}$||$3.3\times 10^{-3}$|0.0|$1.8\times 10^{-5}$||$5.7\times 10^{-4}$||$5.0\times 10^{-4}$|
|$\Sigma$|2.5-Z1-H15004.62.32.02.50.044|$2.9\times 10^{-3}$|0.270.18
|$\Sigma$|2.5-Z1-H20003.60.910.0191.71.80.390.620.56
Table 2.

Summary of results for all runs. All quantities reported here are averaged for |$t\gt 75$| Myr and |$z=L_z$|⁠. Column 2 – the mass loading factor (⁠|$\eta _M$|⁠). Column 3 – the burstiness parameter b (equation 8). Columns 4, 5, and 6 – the contribution to |$\eta _M$| from cool (⁠|$T\lt 2 \times 10^4$| K), warm unstable (⁠|$2 \times 10^4$| K |$\lt T\lt 10^6$| K), and hot (⁠|$T\gt 10^6$| K) gas, respectively. Columns 7 and 8 – the energy loading (⁠|$\eta _E$|⁠) and the metal loading (⁠|$\eta _Z$|⁠) factors. Column 9 – the average fraction of metals promptly lost to the wind rather than retained in the ISM |$\phi$| (equation 7).

Name|$\eta _M$|b|$\eta _M^{\rm cool}$||$\eta _M^{\rm warm}$||$\eta _M^{\rm hot}$||$\eta _E$||$\eta _Z$||$\phi$|
(1)(2)(3)(4)(5)(6)(7)(8)(9)
|$\Sigma$|13-Z1-H1502.11.00.820.311.00.641.00.97
|$\Sigma$|50-Z1-H1500.260.580.00.00.260.970.860.96
|$\Sigma$|2.5-Z1-H1502.32.00.201.690.170.0140.0930.052
|$\Sigma$|13-Z0.2-H1500.0402.7|$1.0\times 10^{-5}$|0.040|$1.4\times 10^{-4}$||$1.3\times 10^{-3}$||$6.0\times 10^{-3}$||$2.7\times 10^{-3}$|
|$\Sigma$|50-Z0.2-H1500.480.650.00.00.480.480.920.89
|$\Sigma$|2.5-Z0.2-H1501.62.10.0811.5|$5.5\times 10^{-3}$|0.0120.034|$4.5\times 10^{-3}$|
|$\Sigma$|2.5-Z1-H3000.282.8|$8.2\times 10^{-4}$|0.27|$7.9\times 10^{-3}$||$8.9\times 10^{-4}$|0.0170.014
|$\Sigma$|2.5-Z1-H1000|$3.2\times 10^{-3}$|3.0|$-2.7 \times 10^{-5}$||$3.3\times 10^{-3}$|0.0|$1.8\times 10^{-5}$||$5.7\times 10^{-4}$||$5.0\times 10^{-4}$|
|$\Sigma$|2.5-Z1-H15004.62.32.02.50.044|$2.9\times 10^{-3}$|0.270.18
|$\Sigma$|2.5-Z1-H20003.60.910.0191.71.80.390.620.56
Name|$\eta _M$|b|$\eta _M^{\rm cool}$||$\eta _M^{\rm warm}$||$\eta _M^{\rm hot}$||$\eta _E$||$\eta _Z$||$\phi$|
(1)(2)(3)(4)(5)(6)(7)(8)(9)
|$\Sigma$|13-Z1-H1502.11.00.820.311.00.641.00.97
|$\Sigma$|50-Z1-H1500.260.580.00.00.260.970.860.96
|$\Sigma$|2.5-Z1-H1502.32.00.201.690.170.0140.0930.052
|$\Sigma$|13-Z0.2-H1500.0402.7|$1.0\times 10^{-5}$|0.040|$1.4\times 10^{-4}$||$1.3\times 10^{-3}$||$6.0\times 10^{-3}$||$2.7\times 10^{-3}$|
|$\Sigma$|50-Z0.2-H1500.480.650.00.00.480.480.920.89
|$\Sigma$|2.5-Z0.2-H1501.62.10.0811.5|$5.5\times 10^{-3}$|0.0120.034|$4.5\times 10^{-3}$|
|$\Sigma$|2.5-Z1-H3000.282.8|$8.2\times 10^{-4}$|0.27|$7.9\times 10^{-3}$||$8.9\times 10^{-4}$|0.0170.014
|$\Sigma$|2.5-Z1-H1000|$3.2\times 10^{-3}$|3.0|$-2.7 \times 10^{-5}$||$3.3\times 10^{-3}$|0.0|$1.8\times 10^{-5}$||$5.7\times 10^{-4}$||$5.0\times 10^{-4}$|
|$\Sigma$|2.5-Z1-H15004.62.32.02.50.044|$2.9\times 10^{-3}$|0.270.18
|$\Sigma$|2.5-Z1-H20003.60.910.0191.71.80.390.620.56
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