- #1
crocomut
- 17
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For a solenoidal velocity field [ tex ] \nabla \cdot \mathbf{u} [ /tex ] which means that [ tex ] \nabla [/tex ] is perpendicular to [ tex ] \mathbf{u} [ /tex ].
Similarly, for an irrotational velocity field [ tex ] \nabla \times \mathbf{u} [ /tex ] which means that [ tex ] \nabla [/tex ] is parallel to [ tex ] \mathbf{u} [ /tex ].
So what exactly does it mean physically to have a gradient (of nothing) parallel/perpendicular to a vector?
PS - what's up with latex not working?
Similarly, for an irrotational velocity field [ tex ] \nabla \times \mathbf{u} [ /tex ] which means that [ tex ] \nabla [/tex ] is parallel to [ tex ] \mathbf{u} [ /tex ].
So what exactly does it mean physically to have a gradient (of nothing) parallel/perpendicular to a vector?
PS - what's up with latex not working?
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