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Basics of Rotating Boundary- Layer Flow NCAR is funded by the National Science Foundation Richard Rotunno NCAR, Boulder CO http://www.mmm.ucar.edu/people/rotunno/
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Page 1: Basics of Rotating Boundary-Layer Flow NCAR is funded by the National Science Foundation Richard Rotunno NCAR, Boulder CO.

Basics of Rotating Boundary-Layer Flow

NCAR is funded by the National Science Foundation

Richard RotunnoNCAR, Boulder CO

http://www.mmm.ucar.edu/people/rotunno/

Page 2: Basics of Rotating Boundary-Layer Flow NCAR is funded by the National Science Foundation Richard Rotunno NCAR, Boulder CO.

Outline

1. Rotating Flow / No Boundary

2. Rotating Flow / Frictional Boundary Layer

3. Boundary Layer of a Solid-Body-Rotation Vortex

4. Boundary Layer of a Potential Vortex

5. Boundary Layer of a Rankine-Type Vortex

6. Summary

Page 3: Basics of Rotating Boundary-Layer Flow NCAR is funded by the National Science Foundation Richard Rotunno NCAR, Boulder CO.

Cylindrical Polar Coordinates

[u,v,w]

[r,φ,z]

z

r

φ

1. Rotating Flow / No Boundary

Page 4: Basics of Rotating Boundary-Layer Flow NCAR is funded by the National Science Foundation Richard Rotunno NCAR, Boulder CO.

Simple Vortex

0 = −∂p

∂r+ρV 2

r€

[0,V (r),0]

z

r

φ

1. Rotating Flow / No Boundary

Page 5: Basics of Rotating Boundary-Layer Flow NCAR is funded by the National Science Foundation Richard Rotunno NCAR, Boulder CO.

http://web.mit.edu/hml/ncfmf.html

2. Rotating Flow/Frictional Boundary layer

Page 6: Basics of Rotating Boundary-Layer Flow NCAR is funded by the National Science Foundation Richard Rotunno NCAR, Boulder CO.

Dye Injected atWater Surface(earlier)

Drain

“Secondary Flow”

2. Rotating Flow/Frictional Boundary layer

Bathtub Vortex

Page 7: Basics of Rotating Boundary-Layer Flow NCAR is funded by the National Science Foundation Richard Rotunno NCAR, Boulder CO.

Dye Injected atWater Surface(later)

Drain

Bathtub Vortex

“Secondary Flow”

2. Rotating Flow/Frictional Boundary layer

Page 8: Basics of Rotating Boundary-Layer Flow NCAR is funded by the National Science Foundation Richard Rotunno NCAR, Boulder CO.

Dye Injected nearBottom (earlier)

Drain

“Secondary Flow”

Bathtub Vortex

2. Rotating Flow/Frictional Boundary layer

Page 9: Basics of Rotating Boundary-Layer Flow NCAR is funded by the National Science Foundation Richard Rotunno NCAR, Boulder CO.

Dye Injected nearBottom (later)

Drain

“Secondary Flow”

Bathtub Vortex

2. Rotating Flow/Frictional Boundary layer

Page 10: Basics of Rotating Boundary-Layer Flow NCAR is funded by the National Science Foundation Richard Rotunno NCAR, Boulder CO.

z

r

φ

z = 0 : u = v = w = 0

2. Rotating Flow/Frictional Boundary layer

0 = −∂p

∂r+ρV 2

r

0 = −∂p

∂r+ν∂ 2u

∂z2

Page 11: Basics of Rotating Boundary-Layer Flow NCAR is funded by the National Science Foundation Richard Rotunno NCAR, Boulder CO.

For any , (radial inflow) near frictional boundary

z

r

φ

V (r)

u < 02. Rotating Flow/Frictional Boundary layer

Page 12: Basics of Rotating Boundary-Layer Flow NCAR is funded by the National Science Foundation Richard Rotunno NCAR, Boulder CO.

Behavior of near frictional boundary depends on

(u,v,w)

V (r)

V ∝ rβ

Similarity solutions exist

Solid-body rotation

Potential vortex

β = 1

β > −1

β =−1

Rott and Lewellen (1966 Prog Aero Sci)

2. Rotating Flow/Frictional Boundary layer

Page 13: Basics of Rotating Boundary-Layer Flow NCAR is funded by the National Science Foundation Richard Rotunno NCAR, Boulder CO.

3. Flow in Solid-Body Rotation Above a Stationary Disk*

* Bödewadt (1940) (Schlichting 1968 Boundary Layer Theory)

V =ωr

Page 14: Basics of Rotating Boundary-Layer Flow NCAR is funded by the National Science Foundation Richard Rotunno NCAR, Boulder CO.

z

νω

3. Flow in Solid-Body Rotation Above a Stationary Disk

Solution exhibits “overshoot” and “pumping”

(vmax >V)

(w(∞) > 0)

Page 15: Basics of Rotating Boundary-Layer Flow NCAR is funded by the National Science Foundation Richard Rotunno NCAR, Boulder CO.

z

νω

3. Flow in Solid-Body Rotation Above a Stationary Disk

u

v

0

0.5

−0.5

1.0

Bödewadt

Ekman

hodograph

Ekman is linearized version of Bödewadt

Page 16: Basics of Rotating Boundary-Layer Flow NCAR is funded by the National Science Foundation Richard Rotunno NCAR, Boulder CO.

3. Flow in Solid-Body Rotation Above a Stationary Disk

0 1 0 1 10-1 -10

z

νω

8

0 ≈ −V

r

2

+ν∂ 2u

∂z2

du

dt≈v 2 −V

r

2

> 0Inertial layer:

Friction layer:

Rotunno and Bryan (Submitted to JAS)

Page 17: Basics of Rotating Boundary-Layer Flow NCAR is funded by the National Science Foundation Richard Rotunno NCAR, Boulder CO.

tangential

radial

3. Flow in Solid-Body Rotation Above a Stationary Disk

LaboratoryExperiment

“Secondary Flow”

Page 18: Basics of Rotating Boundary-Layer Flow NCAR is funded by the National Science Foundation Richard Rotunno NCAR, Boulder CO.

3. Flow in Solid-Body Rotation Above a Stationary Disk

Hurricane Inner-Core Flow

Page 19: Basics of Rotating Boundary-Layer Flow NCAR is funded by the National Science Foundation Richard Rotunno NCAR, Boulder CO.

Zhang, Rogers, Nolan & Marks (2011, Monthly Weather Review)

radial tangential

3. Flow in Solid-Body Rotation Above a Stationary Disk

Composite Dropsonde Analysis of Hurricane Inner-Core Flow

r /rmax

r /rmax

Page 20: Basics of Rotating Boundary-Layer Flow NCAR is funded by the National Science Foundation Richard Rotunno NCAR, Boulder CO.

4. Potential Vortex Above a Stationary Disk: Experiment

V ∝ r−1

Phillips and Khoo (1987, Proc. Roy. Soc. London)

Page 21: Basics of Rotating Boundary-Layer Flow NCAR is funded by the National Science Foundation Richard Rotunno NCAR, Boulder CO.

4. Potential Vortex Above a Stationary Disk: Experiment

V ∝ r−1

Phillips and Khoo (1987, Proc. Roy. Soc. London)

Page 22: Basics of Rotating Boundary-Layer Flow NCAR is funded by the National Science Foundation Richard Rotunno NCAR, Boulder CO.

4. Potential Vortex Above a Stationary Disk: Theory

radial tangential

Burggraf, Stewartson and Belcher (1971, Phys. Fluids)

Radial inflow ( ), but no “overshoot”( )

u < 0

v <V

decreasing radius

decreasing radius

−ru

rv

z

Page 23: Basics of Rotating Boundary-Layer Flow NCAR is funded by the National Science Foundation Richard Rotunno NCAR, Boulder CO.

radial tangential

−ru

rv

102z

r = 0.14. Potential Vortex Above a Stationary Disk: Theory & Experiment

Phillips and Khoo (1987, Proc. Roy. Soc. London)

Page 24: Basics of Rotating Boundary-Layer Flow NCAR is funded by the National Science Foundation Richard Rotunno NCAR, Boulder CO.

radial tangential

−ru

rv

102z

r = 0.14. Potential Vortex Above a Stationary Disk: Theory & Experiment

Phillips and Khoo (1987, Proc. Roy. Soc. London)

0 ≈ −V

r

2

+ν∂ 2u

∂z2

du

dt≈v 2 −V

r

2

< 0

Inertial layer:

Friction layer:

Wilson and Rotunno (1986, Phys. Fluids)

Page 25: Basics of Rotating Boundary-Layer Flow NCAR is funded by the National Science Foundation Richard Rotunno NCAR, Boulder CO.

4. Potential Vortex Above a Stationary Disk: Experiment

Phillips (1985, Proc. Roy. Soc. London)

End-Wall Vortex

Vortex Breakdown

Page 26: Basics of Rotating Boundary-Layer Flow NCAR is funded by the National Science Foundation Richard Rotunno NCAR, Boulder CO.

April 22, 2010 Texas Panhandle (H. Bluestein)

4. Potential Vortex Above a Stationary Disk: Tornado?

Page 27: Basics of Rotating Boundary-Layer Flow NCAR is funded by the National Science Foundation Richard Rotunno NCAR, Boulder CO.

Kuo (1971, JAS)

5. Boundary layer of a Rankine-Type Vortex

V (r)

Page 28: Basics of Rotating Boundary-Layer Flow NCAR is funded by the National Science Foundation Richard Rotunno NCAR, Boulder CO.

Summary Rotating Flow / Frictional Boundary Layer Radial Inflow in BL, if Convergent, Transport from BL to InteriorBoundary Layer of Solid-Body-Rotation VortexApplication: HurricanesBoundary Layer of Potential VortexApplication: Certain Types of TornadoesBoundary Layer of Rankine-Type VortexApplication: Hurricanes& Certain Types of Tornadoes


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