Atmospheric Thermal Structure Flashcards

1
Q

What layer of the atmosphere contains 80% of the total mass of the atmosphere and almost the whole quantity of water vapor?

A

Troposphere

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2
Q

What determines how a pollutant can disperse through the atmosphere?

A

Rate of change of temperature with altitude.

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3
Q

What are the physical properties of the atmosphere (state variables)?

A

Pressure, Density, and temperature.

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4
Q

How is the atmosphere divided into layers?

A

By the vertical distribution of temperature.

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5
Q

T/F: In the troposphere, temperature decreases with height?

A

True

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6
Q

Lapse Rate

A

Γ = -dT/dz

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7
Q

What are the features of the boundary layer?

A
  1. Surface Layer
  2. Convective mixed layer
  3. Temperature Inversion Layer
  4. Residual Layer
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8
Q

What does the boundary layer depend on?

A

Ground temperature

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9
Q

How is a surface inversion created during the night?

A

The ground cools radiatively, causing air temperatures to increase with increasing height from the ground.

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10
Q

T/F: Pollutants are more likely to be trapped in the surface layer at day?

A

False, because the surface inversion causes pollutants to stay trapped.

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11
Q

Ideal gas law specifically for dry air?

A

p = ρd Rd T

  • ρ is rho, density
    Rd = R*/ Md, gas constant
    T = temperature
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12
Q

Ideal gas law for moist air?

A

p = ρv Rd Tv

  • ρ is rho, density
    Rv = R*/Mw
    Tv = virtual temperature
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13
Q

What is virtual temperature tv?

A

The temperature a
hypothetical sample of dry air would need to have in order to have the same density as the sample of moist air at the same pressure.

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14
Q

What is the virtual temperature formula?

A

Tv = [1 + 0.61*rv ] * T

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15
Q

Hydrostatic Equations

A

F pressure = F gravity
−δp = gρδz

At the limit of δz -> 0
∂p/ ∂z = -g*ρ

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16
Q

Hydrostatic balance with ideal gas law:

A

∂p/ ∂z = - p*g/ Rd * Tv

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17
Q

1st law of thermodynamics

A

With Specific heat capacity

dq = cvdT +p

dq = cpdT − αdp

cp = cv + R

Where is cv = 717 JK-1kg-1 and cp = 717 J K-1kg*-1 are the
specific heat at constant volume and pressure respectively.

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18
Q

Isobaric

A

Constant pressure
dp = 0
δq = cp*dT

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19
Q

Isothermal

A

Constant temperature
dT = 0
du = 0 since dT = 0
-> δq = δw
All heat goes into work.

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20
Q

Isochoric

A

Constant volume
dV = 0
δw = 0 since dV = 0 (and dα = 0)
δq = du = cv*dT
No work, all heat into T changes.

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21
Q

Adiabatic

A

No heat exchanged,
δq = 0, du = - δw since δq = 0

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22
Q

How does temperature change with height for a rising thermal?

A

Temperature is the highest when nearer to the ground

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23
Q

Dry adiabatic lapse rate

A

-dT/dz = cp/g = Γd

24
Q

What are the conditions for saturated adiabatic (moist adiabatic)?

A

All condensed water remains in rising air parcel.
No precipitation
Adiabatic - no heat exchanged with environment

25
Saturated Adiabatic lapse rate
Γs - not a constant like dry adiabatic lapse rate Γs - depends on net amount of condensation -dT/dz = Γs = Γd [1 + (Lv+Ws/Rd*T)/ 1+ (Lv^2*ws/Rv*cp*T^2)] Answer in bracket is always smaller than 1, so Γs < Γd
25
Saturated Adiabatic lapse rate
Γs - not a constant like dry adiabatic lapse rate Γs - depends on net amount of condensation -dT/dz = Γs = Γd [1 + (Lv+Ws/Rd*T)/ 1+ (Lv^2*ws/Rv*cp*T^2)] Answer in bracket is always smaller than 1, so Γs < Γd
26
T/F: Saturated lapse rate - Γs- decreases with increasing moisture content (and thus temperature)
True
27
Potential Temperature
θ - as the temperature a parcel would have if it adiabatically moved from existing pressure to a standard pressure, defined as p0 ≡ 1000 hPa.
28
What process is potential temperature?
A conserved adiabatic processes
29
What are the four concepts of stability?
Stable Neutral Unstable Conditionally unstable
30
Stable
Returns to its original position after displacement
31
Neutral
Remains in new position after being displaced
32
Unstable
Moves further away from its original position after being displaced
33
Conditionally unstable
Becomes unstable for a large enough vertical displacement - This is the most common instability in the atmosphere
34
Buoyancy
Ftot = (ρ env + ρ parc)* V*g
35
If density of air parcel (ρparc) is greater than the density of environmental air (ρenv) that it displaces, then the air parcel will experience a . . .
downward directed total (buoyancy + gravity) force (Ftot): ρ parc > ρ env
36
If density of air parcel (ρparc) is less than density of the environmental air (ρenv) that it displaces, then air parcel will experience an . . .
upward directed total (buoyancy + gravity) force (Ftot) ρ parc < ρ env
37
Buoyancy force in terms of T
Parcel’s density immediately adjusts to environment (like a balloon!) - Differences in density are due to differences in T
38
(Ftot = (ρ env + ρ parc)* V*g) + (ρ = p/ Rd Tv)
atot = (Tparc - Tenv / Tparc ) *g
39
Buoyant
T of parcel > T of environment
40
Sink
T of parcel < T of environment
41
Stays put
T of parcel = T of environment
42
What are the three possibilities for saturated air?
Stable Neutral Unstable
43
Characteristics of stable saturated air
Γenv < Γd --> dθ/ dz > 0 -Parcel becomes colder than nearby environment -Downward buoyancy force - Parcel will return to original location
44
Characteristics of neutral saturated air
Γenv = Γd --> dθ/ dz = 0 -Parcel T becomes equal to environment -No buoyancy force - Parcel will remain at new location
45
Characteristics of unstable saturated air
Γenv > Γd --> dθ/ dz < 0 -Parcel becomes warmer than environment -Upward buoyancy force - Parcel will move further away from original location Unsaturated air is unstable if θ decreases with z!
46
What are the 5 possibilities for moist air (either saturated or unsaturated)?
Absolutely unstable Dry neutral Conditionally unstable Moist neutral Absolutely stable
47
Absolutely unstable
Γenv > Γd > Γs Unsaturated parcel becomes warmer than nearby environment Saturated parcel becomes warmer than nearby environment
48
Dry neutral
Γenv = Γd > Γs Unsaturated parcel becomes equivalent to the nearby environment Saturated parcel becomes warmer than nearby environment
49
Conditionally unstable
Γd > Γenv > Γs Unsaturated parcel becomes colder than nearby environment Saturated parcel becomes warmer than nearby environment *The vertical temperature profile at many locations in our atmosphere is conditionally unstable!
50
Moist neutral
Γd > Γenv = Γs Unsaturated parcel becomes colder than nearby environment Saturated parcel becomes equivalent to the nearby environment
51
Absolutely stable
Γd > Γs > Γenv Unsaturated parcel becomes colder than nearby environment Saturated parcel becomes colder than nearby environment
52
At stable atmosphere, what is the application of the source?
fanning
53
At unstable atmosphere, what is the application of the source?
Looping
54
At neutrally stable, what is the application of the source?
Coning
55
At smokestack above the inversion layer, what is the application of the source?
Lofting
56
At smokestack under the inversion layer, what is the application of the source?
Funmigation