Atmospheric 2 Flashcards

1
Q

trace gas transport depends on

A

on
advection and
turbulent mixing

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2
Q

how can atmospheric movement be defined as ?

A

▪ Time-integrated transport
can be approximated by a
set of convection “cells”
▪ Prevailing winds are
easterly in the tropics and
westerly in the
extratropics
– Meteorologists describe
wind direction in terms of
the origin of the air mass
(i.e., westerly = from the
west)

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3
Q

how are green house gases lost?

A

: reaction
with hydroxyl
radical

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4
Q

“Inverse modelling” or “topdown”
▪ Requires:

A

– Atmospheric measurements
– Atmospheric chemical
transport model

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5
Q

what does AGAGE network detect

A

– High-frequency
observations of nonCO2 GHGs

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6
Q

types of emission inference

A

– Global mass balance
– Point source emissions evaluation
➢ “Integrated mass enhancement”, satellite-based methods
➢ Gaussian dispersion models

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7
Q

Trend

A

= sources – sinks

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8
Q

Short-wave infrared (SWIR) satellites used
to detect …

A

solar backscatter More uniform sensitivity across atmospheric column

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9
Q

Thermal infrared (TIR) sensitive to

A

emission from higher in the atmosphere

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10
Q

characteristics of point emissions

A

Estimated that 60% of oil and gas
methane emissions from 10% of
the point sources
* A “heavy-tailed” distribution
* Do not emit continuously, i.e.
“episodic Short Duration, High Impact: , unpredictable

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11
Q

Mass balance

A

▪ Can infer flux by
considering mass of
GHG entering and
leaving airmass

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12
Q

Gaussian dispersion modelling

A

▪ Gases and particles are
dispersed by the wind
(advection) and turbulent, eddy-driven diffusion
▪ When averaged over time,
concentration downwind
resembles a Gaussian
distribution

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13
Q

Gaussian dispersion modelling

A

▪ Assumptions:
– Time averaged concentration (not instantaneous)
– Constant source strength and meteorological conditions
– Constant advection along x-axis (along mean direction of travel)
– Wind speed is much larger than diffusion along the x-axis
– No significant variations in topography
– The pollutant cannot penetrate the ground (total “reflection”)

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14
Q

black body

A

A black body is a theoretical
object that absorbs all
incoming electromagnetic
radiation

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15
Q

Stefan Boltzman law:

A

o Relationship between
temperature and total
energy radiated per unit
area per unit time:

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16
Q

Albedo

A

the fraction of
sunlight that is diffusively
reflected by a body
– 0 = black body (absorbs
everything)
– 1 = white body (reflects
everything)

17
Q

earth as black body

A

At equilibrium, incoming and outgoing flux balance, T0 ~ 255K temperature will be lower

18
Q

black body assumption

A

No Reflectivity: Earth would be darker, absorbing all visible and non-visible light. - albedo
No Atmospheric Effects: No scattering or greenhouse effects, making it colder than the real Earth.
Simplified Energy Balance: The model would not account for climate systems, cloud cover, or feedback mechanisms

19
Q

slab problem

A

In the real atmosphere, GHGs aren’t arranged in a slab. They are distributed
throughout the atmosphere.
– Recall that pressure and density drop with altitude
▪ Infrared radiation is continually absorbed and reemitted, until density drops
sufficiently that photons can escape to space

20
Q

global warming

A

As concentration increases, absorption
increases (α): broadening seen at
edges
▪ More wavelengths emit at lower
temperature: more heat “trapped”
▪ So, CO2 greenhouse effect not caused
by centre of absorption peak getting
stronger, but by broadening of the
peak
▪ Logarithmic dependence of radiative
forcing with concentration

21
Q

Radiative properties:

A

– Must be able to absorb IR
– Is the absorption peak saturated?
-stability

22
Q

Radiative forcing

A

▪ Radiative forcing is the net
change in energy balance
due to some imposed
perturbation
– Expressed in W m-2

23
Q

Potential (GWP)

A

▪ GWP is the radiative
forcing due to a
pulse emission of a
GHG, integrated over
some time horizon,
compared to a pulse
of the same mass of
CO2

24
Q

limiting to the GWP model

A

WP ▪ A pulse of CO2
leads to
a relatively constant
radiative forcing
▪ However, for short
-lived
GHGs (e.g., methane,
~10 year lifetime), the
pulse decays away
▪ Potentially misleading
response of
temperatures to
cumulative CO
2