link author: John von Neumann (via WP:JWB)
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where ''β'' = {{sfrac|∂''f''|∂''y''}} is the variation of the ''Coriolis parameter'' with distance ''y'' in the north–south direction and ''v'' is the component of velocity in this direction. |
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where ''β'' = {{sfrac|∂''f''|∂''y''}} is the variation of the ''Coriolis parameter'' with distance ''y'' in the north–south direction and ''v'' is the component of velocity in this direction. |
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In 1950, Charney, Fjørtoft, and von Neumann integrated this equation (with an added [[diffusion]] term on the [[Left-hand side and right-hand side of an equation|right-hand side]]) on a [[computer]] for the first time, using an observed field of 500 [[pascal (unit)|hPa]] [[geopotential height]] for the first timestep. |
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In 1950, Charney, Fjørtoft, and [[John von Neumann|von Neumann]] integrated this equation (with an added [[diffusion]] term on the [[Left-hand side and right-hand side of an equation|right-hand side]]) on a [[computer]] for the first time, using an observed field of 500 [[pascal (unit)|hPa]] [[geopotential height]] for the first timestep. |
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{{Citation |
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{{Citation |
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| last1 = Charney | first1 = J. G. | last2 = Fjørtoft | first2 = R. |
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| last1 = Charney | first1 = J. G. | last2 = Fjørtoft | first2 = R. |