{"id":691,"date":"2019-12-13T16:58:06","date_gmt":"2019-12-13T20:58:06","guid":{"rendered":"https:\/\/www2.whoi.edu\/site\/aomip\/?page_id=691"},"modified":"2021-06-18T09:21:03","modified_gmt":"2021-06-18T13:21:03","slug":"friction","status":"publish","type":"page","link":"https:\/\/www2.whoi.edu\/site\/aomip\/models\/details\/friction\/","title":{"rendered":"Friction"},"content":{"rendered":"\n\n\t

Friction<\/h1>\n\n\n\n\n\t\n\n\t\n\t\n\t\n\t\n\t\n\t\n\t\n\t\n\t\n\t\n\t\n\t\n\t\n\t\n\t\n\t\n\t\n\t\n\t\n\t\n\t\n\t\n\t\n\t\n\t\n\t\n\t\n\t\n\t\n\t

code<\/p><\/th>

vertical<\/p><\/th>

horizontal<\/p><\/th>

bottom<\/p><\/th>\n<\/tr>\n<\/thead>\n

AWI<\/p><\/td>

constant, 10 cm2\/s<\/p><\/td>

biharmonic, A4=0.5e-21 cm4\/s<\/p><\/td>

quadratic, 1.2e-3<\/p><\/td>\n<\/tr>\n

GSFC<\/p><\/td>

\u00a0Mellor-Yamada 2.5<\/p><\/td>

\u00a0Smagorinski<\/p><\/td>

quadratic<\/p><\/td>\n<\/tr>\n

\u00a0DRAKKAR<\/p><\/td>

\u00a0TKE background 1.e-4 m2\/s<\/p><\/td>

\u00a0Biharmonic\u00a0 A4 = 1.2e10 m4\/s in the Arctic<\/p><\/td>

\u00a0Quadratic\u00a0 1.e-3<\/p><\/td>\n<\/tr>\n

ICMMG<\/p><\/td>

constant, 50 cm2\/s<\/p><\/td>

neptune<\/p><\/td>

linear<\/p><\/td>\n<\/tr>\n

LANL<\/p><\/td>

10 x tracer KPP<\/p><\/td>

biharmonic, A4=1.e20 cm4\/s<\/p><\/td>

quadratic, 1.22e-3<\/p><\/td>\n<\/tr>\n

LU<\/p><\/td>

neptune, 300 cm2\/s<\/p><\/td>

neptune, L=3.5e3 m, A2=5e8 cm2\/s<\/p><\/td>

quadratic, 1.2e-3<\/p><\/td>\n<\/tr>\n

NERSC<\/p><\/td>

10 x background tracer<\/p><\/td>

laplacian<\/p><\/td>

quadratic<\/p><\/td>\n<\/tr>\n

NPS<\/p><\/td>

Pacanowski & Philander<\/p><\/td>

biharmonic, A4=1.e-19 cm4\/s<\/p><\/td>

\u00a0<\/p><\/td>\n<\/tr>\n

NYU<\/p><\/td>

interlayer, 1.e-5 m\/s2<\/p><\/td>

laplacian, propto grid space<\/p><\/td>

quadratic<\/p><\/td>\n<\/tr>\n

POL<\/p><\/td>

KPP + constant 10cm2\/s<\/p><\/td>

neptune + Smagorinsky<\/p><\/td>

none<\/p><\/td>\n<\/tr>\n

FEMAO1<\/p><\/td>

Constant 10.0 cm2\/s, or Monin-Obukhov > 1.0 cm2\/s, or<\/p>
\n

1.5L turbulence scheme<\/p><\/td>

Neptune+Laplacian, A2=1.e4 m2\/s<\/p><\/td>

quadratic, 1.0e-3<\/p><\/td>\n<\/tr>\n

FEMAO2<\/p><\/td>

Constant 10.0 cm2\/s, or Monin-Obukhov > 1.0 cm2\/s, or<\/p>
\n

1.5L turbulence scheme<\/p><\/td>

Neptune+Laplacian<\/p><\/td>

quadratic, 1.0e-3<\/p><\/td>\n<\/tr>\n

INMOM<\/p><\/td>

Kochergin, Monin, Obukhov, 1 cm2\/s<\/p><\/td>

biharmonic, A4~1.e-19 cm4\/s<\/p><\/td>

quadratic, 2.5e-3<\/p><\/td>\n<\/tr>\n

RCO<\/p><\/td>

k-epsilon (Meier, 2001)<\/p><\/td>

laplacian 5.e3 m2\/s<\/p><\/td>

quadratic 1.25e-3<\/p><\/td>\n<\/tr>\n

UCL<\/p><\/td>

1.5L turbulence scheme<\/p><\/td>

laplacian, A2=4.e4 m2\/s<\/p><\/td>

linear, 115day<\/p><\/td>\n<\/tr>\n

UW<\/p><\/td>

constant, 0.05 cm2\/s<\/p><\/td>

laplacian, A2=1.2e8 cm2\/s<\/p><\/td>

none<\/p><\/td>\n<\/tr>\n

DAL<\/p><\/td>

\u00a0<\/p><\/td>

\u00a0<\/p><\/td>

\u00a0<\/p><\/td>\n<\/tr>\n

FSU<\/p><\/td>

\u00a0<\/p><\/td>

\u00a0<\/p><\/td>

\u00a0<\/p><\/td>\n<\/tr>\n

GFDL<\/p><\/td>

\u00a0<\/p><\/td>

\u00a0<\/p><\/td>

\u00a0<\/p><\/td>\n<\/tr>\n

IARC-A<\/p><\/td>

constant 1.e-4 m2\/s<\/p><\/td>

laplacian, A2=5.e3 m2\/s<\/p><\/td>

quadratic, 1.e-3<\/p><\/td>\n<\/tr>\n

IARC-B<\/p><\/td>

constant 1.e-4 m2\/s<\/p><\/td>

Smagorinsky biharmonic, C=3<\/p><\/td>

quadratic, 1.e-3<\/p><\/td>\n<\/tr>\n

ECCO2<\/p><\/td>

5.661e-4 m2\/s<\/p><\/td>

modified Leigh (Fox-Kemper & Menemenlis, 2008)<\/p><\/td>

no-slip, quadratic, 2.1e-3<\/p><\/td>\n<\/tr>\n

MIT<\/p><\/td>

\u00a0<\/p><\/td>

\u00a0<\/p><\/td>

\u00a0<\/p><\/td>\n<\/tr>\n

NCAR<\/p><\/td>

\u00a0<\/p><\/td>

\u00a0<\/p><\/td>

\u00a0<\/p><\/td>\n<\/tr>\n

NPI<\/p><\/td>

\u00a0<\/p><\/td>

\u00a0<\/p><\/td>

\u00a0<\/p><\/td>\n<\/tr>\n

UMASD<\/p><\/td>

\u00a0<\/p><\/td>

\u00a0<\/p><\/td>

\u00a0<\/p><\/td>\n<\/tr>\n

NOCS\/ORCA25<\/p><\/td>

TKE+enhanced 1.e-4 m2\/s<\/p><\/td>

bi-harmonic (-1.5e-11 m\/2s)<\/p><\/td>

quadratic + local enhancement<\/p><\/td>\n<\/tr>\n

MCGU<\/p><\/td>

\u00a0<\/p><\/td>

\u00a0<\/p><\/td>

\u00a0<\/p><\/td>\n<\/tr>\n

LOCEAN<\/p><\/td>

Gaspar et al., 1990<\/p><\/td>

biharmonic : -8.5e+11<\/p><\/td>

non-linear<\/p><\/td>\n<\/tr>\n

IOS<\/p><\/td>

neptune, up to 1 m2\/s<\/p><\/td>

neptune, L=3.5e3 m, A2=4.e4 m2\/s<\/p><\/td>

quadratic, 1.2e-3<\/p><\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n\n\n","protected":false},"excerpt":{"rendered":"

Friction<\/p>\n","protected":false},"author":83,"featured_media":0,"parent":639,"menu_order":8,"comment_status":"closed","ping_status":"closed","template":"tpl-sidebar.php","meta":{"advanced-sidebar-menu\/link-title":"","advanced-sidebar-menu\/exclude-page":false},"_links":{"self":[{"href":"https:\/\/www2.whoi.edu\/site\/aomip\/wp-json\/wp\/v2\/pages\/691"}],"collection":[{"href":"https:\/\/www2.whoi.edu\/site\/aomip\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/www2.whoi.edu\/site\/aomip\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/www2.whoi.edu\/site\/aomip\/wp-json\/wp\/v2\/users\/83"}],"replies":[{"embeddable":true,"href":"https:\/\/www2.whoi.edu\/site\/aomip\/wp-json\/wp\/v2\/comments?post=691"}],"version-history":[{"count":3,"href":"https:\/\/www2.whoi.edu\/site\/aomip\/wp-json\/wp\/v2\/pages\/691\/revisions"}],"predecessor-version":[{"id":1676,"href":"https:\/\/www2.whoi.edu\/site\/aomip\/wp-json\/wp\/v2\/pages\/691\/revisions\/1676"}],"up":[{"embeddable":true,"href":"https:\/\/www2.whoi.edu\/site\/aomip\/wp-json\/wp\/v2\/pages\/639"}],"wp:attachment":[{"href":"https:\/\/www2.whoi.edu\/site\/aomip\/wp-json\/wp\/v2\/media?parent=691"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}