초록 ▼

An apparatus delays the transition of a boundary layer flow from laminar to turbulent. Flow disruptors are positioned to be in contact with a boundary layer flow moving in a flow direction over a surface. Each flow disruptor generates fluctuations in the boundary layer flow such that the frequency o

An apparatus delays the transition of a boundary layer flow from laminar to turbulent. Flow disruptors are positioned to be in contact with a boundary layer flow moving in a flow direction over a surface. Each flow disruptor generates fluctuations in the boundary layer flow such that the frequency of the fluctuations is a damping region frequency defined by an amplification rate curve associated with the boundary layer flow.

대표청구항 ▼

1. An apparatus for delaying the transition of a boundary layer flow from laminar to turbulent, comprising: a plurality of flow disruptors adapted to be in contact with a boundary layer flow moving in a flow direction over a surface, each of said flow disruptors generating fluctuations in the bounda

1. An apparatus for delaying the transition of a boundary layer flow from laminar to turbulent, comprising: a plurality of flow disruptors adapted to be in contact with a boundary layer flow moving in a flow direction over a surface, each of said flow disruptors generating fluctuations in the boundary layer flow at a frequency that is a damping region frequency defined by an amplification rate curve associated with the boundary layer flow. 2. An apparatus as in claim 1, wherein said plurality of flow disruptors are arranged approximately perpendicular to the flow direction of the boundary layer flow. 3. An apparatus as in claim 1, wherein each of said flow disruptors comprises a physical structure adapted to be coupled to the surface and extending only partially into the boundary layer flow. 4. An apparatus as in claim 3, wherein said physical structure comprises a shape selected from the group consisting of spherical shapes, conical shapes, triangular shapes, rectangular shapes and polygonal shapes. 5. An apparatus as in claim 4, wherein said frequency of said fluctuations satisfies the relationship S(U/d) where S is the Strouhal number, U is the flow velocity of the boundary layer flow at said spherical shapes, and d is the diameter of said spherical shapes. 6. An apparatus as in claim 2, wherein said plurality of flow disruptors comprises a plurality of longitudinally-extending parallel ridges. 7. An apparatus as in claim 6, wherein said frequency of said fluctuations satisfies the relationship U/s where U is the flow velocity of the boundary layer flow across peaks of said ridges and s is the distance between adjacent ones of said peaks. 8. An apparatus as in claim 1, wherein each of said flow disruptors comprises a plasma discharge element adapted to be mounted in the surface and flush therewith. 9. An apparatus for delaying the transition of a boundary layer flow from laminar to turbulent, comprising: a plurality of flow disruptors adapted to be in contact with a boundary layer flow moving at a velocity in a flow direction over a surface and arranged approximately perpendicular to the flow direction, each of said flow disruptors generating fluctuations in the boundary layer flow at a frequency that is a damping region frequency defined by an amplification rate curve associated with the boundary layer flow at the velocity. 10. An apparatus as in claim 9, wherein each of said flow disruptors comprises a physical structure adapted to be coupled to the surface and extending only partially into the boundary layer flow. 11. An apparatus as in claim 10, wherein said physical structure comprises a shape selected from the group consisting of spherical shapes, conical shapes, triangular shapes, rectangular shapes and polygonal shapes. 12. An apparatus as in claim 11, wherein said frequency of said fluctuations satisfies the relationship S(U/d) where S is the Strouhal number, U is the velocity of the boundary layer flow at said spherical shapes, and d is the diameter of said spherical shapes. 13. An apparatus as in claim 9, wherein said plurality of flow disruptors comprises a plurality of longitudinally-extending parallel ridges. 14. An apparatus as in claim 13, wherein said frequency of said fluctuations satisfies the relationship U/s where U is the velocity of the boundary layer flow across peaks of said ridges and s is the distance between adjacent ones of said peaks. 15. An apparatus as in claim 9, wherein each of said flow disruptors comprises a plasma discharge element adapted to be mounted in the surface and flush therewith. 16. An apparatus for delaying the transition of a boundary layer flow from laminar to turbulent, comprising: a plurality of flow disruptors adapted to be in contact with a boundary layer flow moving at a velocity in a flow direction over a surface and arranged approximately perpendicular to the flow direction, each of said flow disruptors generating fluctuations in the boundary layer flow at a frequency that is a damping region frequency defined by an amplification rate curve associated with the boundary layer flow at the velocity; andeach of said flow disruptors selected from the group consisting of (i) a physical structure adapted to be coupled to the surface and extending only partially into the boundary layer flow, and (ii) a plasma discharge element adapted to be mounted in the surface and flush therewith. 17. An apparatus as in claim 16, wherein said physical structure comprises a shape selected from the group consisting of spherical shapes, conical shapes, triangular shapes, rectangular shapes and polygonal shapes. 18. An apparatus as in claim 17, wherein said frequency of said fluctuations satisfies the relationship S(U/d) where S is the Strouhal number, U is the velocity of the boundary layer flow at said spherical shapes, and d is the diameter of said spherical shapes. 19. An apparatus as in claim 16, wherein said physical structure comprises longitudinally-extending parallel ridges. 20. An apparatus as in claim 19, wherein said frequency of said fluctuations satisfies the relationship U/s where U is the velocity of the boundary layer flow across peaks of said ridges and s is the distance between adjacent ones of said peaks.