| 11. | Here, the projections are accomplished by the orthogonality of the solenoidal and irrotational function spaces.
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| 12. | Because the flow is irrotational, the wave motion can be described using potential flow theory.
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| 13. | In a simply connected open region, an irrotational vector field has the path-independence property.
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| 14. | For an irrotational flow, the flow velocity can be described as the gradient of a velocity potential.
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| 15. | An irrotational flow means the velocity field is conservative, or equivalently the vorticity pseudovector field is zero:
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| 16. | Here, we will use a inviscid and incompressible, and the flow is assumed to be irrotational.
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| 17. | In fluid dynamics, it is often referred to as a vortex-free or irrotational vector field.
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| 18. | Kelvin's circulation theorem states that a fluid that is irrotational in an inviscid flow will remain irrotational.
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| 19. | Kelvin's circulation theorem states that a fluid that is irrotational in an inviscid flow will remain irrotational.
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| 20. | Use is made of the fluid being incompressible and its flow is irrotational ( often, sensible approximations ).
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