191 | | ||[[span(w*e* ,style=color: green)]] ||Vertical flux of perturbation energy (resolved) ||m^3^/s^3^ || |
192 | | ||[[span(u*2 ,style=color: blue)]] ||Variance of the u-velocity component (resolved) ||m^2^/s^2^ || |
193 | | ||[[span(v*2 ,style=color: blue)]] ||Variance of the v-velocity component (resolved) ||m^2^/s^2^ || |
194 | | ||[[span(w*2 ,style=color: green)]] ||Variance of the w-velocity component (resolved) ||m^2^/s^2^ || |
195 | | ||[[span(pt*2 ,style=color: blue)]] ||Variance of the potential temperature (resolved) ||K^2 || |
196 | | ||[[span(w*3 ,style=color: green)]] ||Third moment of the w-velocity component (resolved) ||m^3^/s^3^ || |
197 | | ||[[span(Sw ,style=color: green)]] ||Skewness of the w-velocity component (resolved, Sw = w^3^ / (w^2^)^1.5^) ||m^3^ / s^3/(m^2^/s^2^)^1.5^ || |
198 | | w*2pt* Third moment (resolved) |
199 | | w*pt*2 Third moment (resolved) |
200 | | w*u*u*:dz Energy production by shear (resolved) |
201 | | w*p*:dz Energy production by turbulent transport of pressure fluctuations (resolved) |
202 | | w"e:dz Energy production by transport of resolved-scale TKE |
203 | | hyp Hydrostatic pressure (in dbar) |
| 191 | ||[[span(w*e* ,style=color: green)]] ||Vertical flux of perturbation energy (resolved) || || |
| 192 | ||[[span(u*2 ,style=color: blue)]] ||Variance of the u-velocity component (resolved) || || |
| 193 | ||[[span(v*2 ,style=color: blue)]] ||Variance of the v-velocity component (resolved) || || |
| 194 | ||[[span(w*2 ,style=color: green)]] ||Variance of the w-velocity component (resolved) || || |
| 195 | ||[[span(pt*2 ,style=color: blue)]] ||Variance of the potential temperature (resolved) || || |
| 196 | ||[[span(w*3 ,style=color: green)]] ||Third moment of the w-velocity component (resolved) || || |
| 197 | ||[[span(Sw ,style=color: green)]] ||Skewness of the w-velocity component (resolved, Sw = w^3^/(w^2^)^1.5^) || || |
| 198 | ||[[span(w*2pt* ,style=color: green)]] ||Third moment (resolved) || || |
| 199 | ||[[span(w*pt*2 ,style=color: green)]] ||Third moment (resolved) || || |
| 200 | ||[[span(w*u*u*:dz ,style=color: blue)]] ||Energy production by shear (resolved) || || |
| 201 | ||[[span(w*p*:dz ,style=color: blue)]] ||Energy production by turbulent transport of pressure fluctuations (resolved) || || |
| 202 | ||[[span(w"e:dz ,style=color: blue)]] ||Energy production by transport of resolved-scale TKE || || |
| 203 | ||[[span(hyp ,style=color: blue)]] ||Hydrostatic pressure ||dbar || |
| 204 | \\\\ |
| 205 | Beyond that, initial profiles (t=0) of some variables can additionally be output (this output is only done once with the first plot output and not repeated with the profile output at later times). The names of these profiles result from the ones specified above leaded by a hash "#". Allowed values are:\\\\ |
| 206 | #u, #v, #pt, #km, #kh, #l, #lpt, #q, #qv, #s, #sa, #vpt\\\\ |
| 207 | Profile names preceded by a hash automatically imply that profiles for these variables are also output at later times. It is not necessary and not allowed to specify the same profile name with and without hash simultaneously(this would lead to an NetCDF error). |