Chapter 3 Flashcards

1
Q

Turbulence statistics differ case by case because of

A
  • different surface forcing,
  • geostrophic wind, or
  • different sounding
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2
Q

Turbulence statistics differ case by case because of different surface forcing,

geostrophic wind, or different sounding.

 But with proper …………….., most turbulent statistics of the PBL collapse onto some ……………….

A

scaling

universal curves, even though data are taken from different cases.

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3
Q

Turbulence statistics differ case by case because of different surface forcing, geostrophic wind, or different sounding.

 But with proper scaling, most turbulent statistics of the PBL collapse onto some universal curves, even though data are taken from different cases.

 In other words, ………………

A

if we can come up with proper scaling parameters, turbulent statistics obtained from a wide range of meteorological conditions can be normalized in such a way that their non‐dimensional statistics are similar.

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4
Q

Employing typical characteristic ……………………………enables us to derive …………………………….

A

length, time, and velocity scales

governing equations in a non‐dimensional form.

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5
Q

Employing typical characteristic length, time, and velocity scales enables us to derive governing equations in a non‐dimensional form.

 The advantage is that we can

A

compare the relative importance of each contribution and reduce the number of parameters needed to study the atmospheric flow

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6
Q

Variables that frequently appear in combination with one another are grouped to form

A

new variables that may be nondimensional, such as the Richardson number,

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7
Q

Variables having simple dimensional units such as

A

velocity, length, or time in some cases are related to the most important scales of motion in the eddies

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8
Q

Turbulence Scales

A
  • length scales
  • Velocity scaales
    • deardoff velocity scale (w*)
    • Friction velocity scale (u*)
  • time scales
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9
Q

length scales

A
  • Altitude of the capping inversion, zi,
    • for the whole boundary layer
    • for statically unstable and neutral conditions.
  • Aerodynamic roughness length z0
    • for the surface layer (bottom 5% of PBL)
    • indicates the roughness of the surface
  • Obukhov lenght (L)
    • for statistically nonneutral conditions in the surface layer
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10
Q

Obukhov length (L)

A
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11
Q

Velocity Scales

A
  • Deardorff velocity scale (w*)
    • characterizing the turbulent mixing due to free convection in an unstably stratified BL
  • Friction velocity velocity scale (u*)
    • applicable to statically neutral conditions in the surface layer (the turbulence is mostly mechanically generated)
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12
Q

Deardorff velocity scale (w*) ‐

A
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13
Q

Friction velocity scale ‐ Another scale u*,

A
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14
Q

Time Scales

A
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15
Q

In summary, For convective boundary layers (ie………..) the relevant scaling parameters are ………….

A

(ie., unstable mixed layers)

w* and Zi

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16
Q

For the neutral surface layer, ……………… are applicable.

A

u* and z0

17
Q

Scaling parameters for surface layers are

A

u*, z0, and L, provided that the stratification is not neutral.

18
Q

Scaling laws describe

A

the functional relationship between two physical quantities that scale with each other over a significant interval.

19
Q

Scaling laws describe the functional relationship between two physical quantities that scale with each other over a significant interval.

 An example of this is

A

the scaling law for wind profile in the ABL

20
Q

Wind profile ‐ the wind profile law

A
21
Q

For non‐neutral situations. the wind profile

A

deviates slightly from logarithmic.

22
Q

In stable boundary layers. the wind profile

A

is concave downward on a semi log plot

23
Q

unstable boundary layers wind profile

A

are concave upward

24
Q

Air stability refers to

A

the vertical moving tendency of an air parcel in response to a small disturbance.

25
Q

The amplification of a small vertical disturbance in an…………… atmosphere, represents the …………………………..

A

unstable

mechanism by which buoyancy produces turbulence

26
Q

Under neutral conditions, turbulence is generated

A

mechanically by wind shear

27
Q

the flow is dynamically unstable when

A

the presence of wind shear and a viscous force

such that a small initial perturbation will become amplified, leading to overturning motion.