Table 5.

Standard enthalpies of reaction at 300 K and the corresponding thresholds of wavelength for the dissociation of gaseous methane into other atomic and molecular species in their ground states, except CH2 also in excited state.

ΔrHo/kJ mol−1λthreshold/ nm
CH4 + hv → CH3 + H442270.5(1a)
|$\phantom{{\rm CH}_4 + hv} \to {\rm CH}_{\rm 2} {\rm X} + {\rm H}_2$|466.5256.4(1b)
|$\phantom{{\rm CH}_4 + hv}\to {\rm CH}_2 \;a + {\rm H}_2$|518.6230.7(1c)
|$\phantom{{\rm CH}_4 + hv} \to {\rm CH}_2 \,{\rm X} + 2{\rm H}$|902.5132.5(1d)
|$\phantom{{\rm CH}_4 + hv} \to {\rm CH} + {\rm H} + {\rm H}_{\rm 2}$|887134.8(1e)
|$\phantom{{\rm CH}_4 + hv} \to {\rm CH} + 3{\rm H}$|132390.4(1f)
|$\phantom{{\rm CH}_4 + hv} \to {\rm C} + 2{\rm H}_2$|791.5151.1(1g)
|$\phantom{{\rm CH}_4 + hv} \to {\rm C} + 4{\rm H}$|166471.9(1h)
ΔrHo/kJ mol−1λthreshold/ nm
CH4 + hv → CH3 + H442270.5(1a)
|$\phantom{{\rm CH}_4 + hv} \to {\rm CH}_{\rm 2} {\rm X} + {\rm H}_2$|466.5256.4(1b)
|$\phantom{{\rm CH}_4 + hv}\to {\rm CH}_2 \;a + {\rm H}_2$|518.6230.7(1c)
|$\phantom{{\rm CH}_4 + hv} \to {\rm CH}_2 \,{\rm X} + 2{\rm H}$|902.5132.5(1d)
|$\phantom{{\rm CH}_4 + hv} \to {\rm CH} + {\rm H} + {\rm H}_{\rm 2}$|887134.8(1e)
|$\phantom{{\rm CH}_4 + hv} \to {\rm CH} + 3{\rm H}$|132390.4(1f)
|$\phantom{{\rm CH}_4 + hv} \to {\rm C} + 2{\rm H}_2$|791.5151.1(1g)
|$\phantom{{\rm CH}_4 + hv} \to {\rm C} + 4{\rm H}$|166471.9(1h)
Table 5.

Standard enthalpies of reaction at 300 K and the corresponding thresholds of wavelength for the dissociation of gaseous methane into other atomic and molecular species in their ground states, except CH2 also in excited state.

ΔrHo/kJ mol−1λthreshold/ nm
CH4 + hv → CH3 + H442270.5(1a)
|$\phantom{{\rm CH}_4 + hv} \to {\rm CH}_{\rm 2} {\rm X} + {\rm H}_2$|466.5256.4(1b)
|$\phantom{{\rm CH}_4 + hv}\to {\rm CH}_2 \;a + {\rm H}_2$|518.6230.7(1c)
|$\phantom{{\rm CH}_4 + hv} \to {\rm CH}_2 \,{\rm X} + 2{\rm H}$|902.5132.5(1d)
|$\phantom{{\rm CH}_4 + hv} \to {\rm CH} + {\rm H} + {\rm H}_{\rm 2}$|887134.8(1e)
|$\phantom{{\rm CH}_4 + hv} \to {\rm CH} + 3{\rm H}$|132390.4(1f)
|$\phantom{{\rm CH}_4 + hv} \to {\rm C} + 2{\rm H}_2$|791.5151.1(1g)
|$\phantom{{\rm CH}_4 + hv} \to {\rm C} + 4{\rm H}$|166471.9(1h)
ΔrHo/kJ mol−1λthreshold/ nm
CH4 + hv → CH3 + H442270.5(1a)
|$\phantom{{\rm CH}_4 + hv} \to {\rm CH}_{\rm 2} {\rm X} + {\rm H}_2$|466.5256.4(1b)
|$\phantom{{\rm CH}_4 + hv}\to {\rm CH}_2 \;a + {\rm H}_2$|518.6230.7(1c)
|$\phantom{{\rm CH}_4 + hv} \to {\rm CH}_2 \,{\rm X} + 2{\rm H}$|902.5132.5(1d)
|$\phantom{{\rm CH}_4 + hv} \to {\rm CH} + {\rm H} + {\rm H}_{\rm 2}$|887134.8(1e)
|$\phantom{{\rm CH}_4 + hv} \to {\rm CH} + 3{\rm H}$|132390.4(1f)
|$\phantom{{\rm CH}_4 + hv} \to {\rm C} + 2{\rm H}_2$|791.5151.1(1g)
|$\phantom{{\rm CH}_4 + hv} \to {\rm C} + 4{\rm H}$|166471.9(1h)
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