institute for climate and atmospheric science balloons, waves and cirrus in the tropics steven...

57
Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University of Leeds Sardar Al-Jumur Benjamin Murray, Theodore Wilson, Zhiqiang Cui Ottmar Möhler, Martin Schnaiter, Robert Wagner, Stefan Benz, Monika Niemand, Harald Saathoff, Volker Ebert, Steven Wagner and Bernd Kärcher Neil Gordon MOGUL Meeting – Feb 28, 2013

Upload: reginald-blake

Post on 18-Jan-2016

214 views

Category:

Documents


0 download

TRANSCRIPT

Page 1: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Institute for Climate and Atmospheric Science

Balloons, waves and cirrus in the tropics

Steven Dobbie

Institute for Climate and Atmospheric ScienceUniversity of Leeds

Sardar Al-Jumur

Benjamin Murray, Theodore Wilson, Zhiqiang Cui

Ottmar Möhler, Martin Schnaiter, Robert Wagner, Stefan Benz, Monika Niemand, Harald Saathoff, Volker Ebert, Steven Wagner and

Bernd Kärcher

Neil Gordon

MOGUL Meeting – Feb 28, 2013

Page 2: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Institute for Climate and Atmospheric Science

Balloons, waves and cirrus in the tropics

Page 3: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Institute for Climate and Atmospheric Science

What is interesting about TTL region?

Ice supersaturations frequently exceed 100% Rhi

(Jensen et al, 2005; Peter et al., 2006).

Is something inhibiting the formation of cirrus?

Page 4: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Institute for Climate and Atmospheric Science

What is interesting about thin TTL cirrus?

High in-cloud supersaturations and low ice number concentrations

(Kramer et al., 2009)

Why aren’t high supersaturations in cloud being quenched?

Page 5: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Institute for Climate and Atmospheric Science

“Supersaturation puzzle”

Page 6: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Institute for Climate and Atmospheric Science

Source of supersaturation

- As air rises the air cools and RHice rises

Sink of supersaturation

- As RHice rises vapour deposits on ice crystals present

Page 7: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Institute for Climate and Atmospheric Science

- Homogeneous nucleation results in numerous crystals of small size so RHice is quenched quickly

- Heterogeneous nucleation results in few crystals of larger size and RHice is slower to quench.

- Numbers of traditional IN are too few

Page 8: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Institute for Climate and Atmospheric Science

Page 9: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Institute for Climate and Atmospheric Science

Page 10: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Institute for Climate and Atmospheric Science

What is up there?

Froyd et al 2010:

Page 11: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Institute for Climate and Atmospheric Science

Candidates?

-Mineral dust?

- Low numbers

“Even if all mineral dust nucleated they couldn’t explain the ice numbers” (Froyd et al 2010)

Page 12: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Institute for Climate and Atmospheric Science

What if?

What if some of the numerous solution aerosols were nucleating at lower super-saturations—below water saturation?

Page 13: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Institute for Climate and Atmospheric Science

Candidates?

Sulphates crystallise in low relative humidity conditions.

- numbers are high

- solid so could act as an ice nuclei?

Page 14: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Institute for Climate and Atmospheric Science

Candidates?

- Sulphates are too viscous at TTL conditions to crystallise (Bodsworth et al., 2010)

Page 15: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Institute for Climate and Atmospheric Science

Candidates?

-Very low accommodation coefficient (0.0075) and so slow uptake of water vapour? (Magee et al., 2006)

-Recent work by Skrotzki (2012) shows it is > 0.1

Page 16: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Institute for Climate and Atmospheric Science

Candidates?

What else could be solid and act as an IN at low temperatures?

Page 17: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Institute for Climate and Atmospheric Science

Glassy aerosols

”Temperature at which materials change from hard and brittle to soft and pliable”

“The temperature below which an amorphous material is a glassy solid and above which it is a viscous liquid“

Murray et al., 2008 and Zobrist et al., 2008

Previously not thought to be applicable to troposphere but is relevant for TTL.

Thought to potentially inhibit nucleation

Page 18: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Institute for Climate and Atmospheric Science

Brittle glassy aerosol

T / RHi decreasing

Laboratory glassy aerosols

Page 19: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Institute for Climate and Atmospheric Science

Brittle glassy aerosol Liquid solution aerosol

T / RHi increasing

Page 20: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Institute for Climate and Atmospheric Science

AIDA Chamber, Karlsruhe Aqueous citric acid,

Raffinose/M5AS,

Levoglucosan,

HMMA

i) it has similar functionality to oxygenated organic

compounds known to exist in atmospheric aerosols;

ii) its glass forming properties are similar to a range of other atmospherically relevant aqueous organic solutions and aqueous organic-sulphate mixtures; and

iii) Representative of products found in the atmosphere.

Page 21: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Institute for Climate and Atmospheric Science

What did the AIDA results show for glassy behaviour during nucleation?

Page 22: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Institute for Climate and Atmospheric Science

AIDA results:

Above 212K

(non-glassy regime)

Below 212K

(glassy regime)

Page 23: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Institute for Climate and Atmospheric Science

AIDA results:

Above 212K

(non-glassy regime)

Below 212K

(glassy regime)

Page 24: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Institute for Climate and Atmospheric Science

Modelling results

1-D APSC (Karcher, DLR) runs:

185 190 195

16.6

16.8

17.0

17.2

17.4

17.6

17.8

18.0

80 90 100 0 20 40 60 80 100 0 1 2 3 4

Alti

tude

/ km

Temperature / K Pressure / mBar RHi (%)

H2O mixing ratio

/ ppm

Page 25: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Institute for Climate and Atmospheric Science

0 100 200 300100

110

120

130

140

150

160

0.0

0.1

0.2

0.3

0.4

0.5

0.6

0.00

0.02

0.04

0.06

0.08

0.10

0.12

0.14

0.16

0.18

0.20

0.22

0

1

2

3

4

5

6

7

8

9

10

11

0 100 200 300

b) HET

(%)RHi

IWC

Nice

(%)R

Hi

Time / minutes

a) HOM

Nic

e / cm

-3

Nice

IWC

IWC

/ m

g m

-3

(%)RHi

R / m

R

Time / minutes

R

APSC results: Constant uplift

b) Glassy

Page 26: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Institute for Climate and Atmospheric Science

0 100 200 300 400100

110

120

130

140

150

160

0 100 200 300 400

0.01

0.1

1HOM, 0.76 K hr-1

3.8 K hr-1

3.8 K hr-1

2.5 K hr-1

1.26 K hr-1

0.25 K hr-1

0.76 K hr-1

0.50 K hr-1

HOM, 0.76 K hr-1

% R

Hi

Time / minutes

0.25 K hr-1

0.50 K hr-10.76 K hr-1 1.26 K hr-1

2.5 K hr-1

Nic

e /

cm-3

Time / minutes

Me

asu

red

Nic

e

APSC results: Citric acid/constant uplift

Page 27: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Institute for Climate and Atmospheric Science

APSC results: Raffinose/M5AS

Page 28: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Institute for Climate and Atmospheric Science

IN indirect response

Page 29: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Institute for Climate and Atmospheric Science

Glassy indirect effect

Page 30: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Institute for Climate and Atmospheric Science

Page 31: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Institute for Climate and Atmospheric Science

Forced by single waves: het/glassy

Page 32: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Institute for Climate and Atmospheric Science

Page 33: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Institute for Climate and Atmospheric Science

Forced by observed

superposition of waves:

(Jensen and Pfister, 2004)

Page 34: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Institute for Climate and Atmospheric Science

Deposition coefficient sensitivity

Page 35: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Institute for Climate and Atmospheric Science

High altitude balloon observations (Hertzog et al., LMD)

- 2-3 months floating around in the tropics

advected on constant density surfaces

- measuring temperature and pressure

Page 36: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Institute for Climate and Atmospheric Science

High altitude balloon (LMD; Hertzog et al)- 2-3 months floating around in the tropics

advected on constant density surfaces

- measuring temperature and pressure

Page 37: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Institute for Climate and Atmospheric Science

Hertzog et al

Balloon trajectory

Page 38: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Institute for Climate and Atmospheric Science

Temperature variations

Page 39: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Institute for Climate and Atmospheric Science

Het (glassy) model run

Page 40: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Institute for Climate and Atmospheric Science

Page 41: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Institute for Climate and Atmospheric Science

Hom activated

Page 42: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Institute for Climate and Atmospheric Science

Optical depth

Page 43: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Institute for Climate and Atmospheric Science

Cloud lifetime

Hom Glassy

Page 44: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Institute for Climate and Atmospheric Science

Radiative properties

Page 45: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Institute for Climate and Atmospheric Science

Satellite observations

Can we obtain remote sensing at the location of the balloon?

Page 46: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Institute for Climate and Atmospheric Science

Satellite observations

Page 47: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Institute for Climate and Atmospheric Science

MLS – AURA CALIPSO - Lidar

Page 48: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Conclusions

Experiments:

- A range of common organics and organic/sulphate mixtures become glassy and nucleate ice heterogeneously

Modelling:

- Modelling results using glassy aerosols are consistent with observed high in-cloud super-saturations and low ice number concentrations

- Modelling agree for ice number, RHi, optical depth, heating rates, etc.

Institute for Climate and Atmospheric Science

Page 49: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Conclusions

Modelling:

- Consistency for both constant lifting and gravity waves forcings

- Strong potential indirect response with glassy nucleation

- Suppression of ice number

- Shorter lifetime

- Heterogeneous nucleation mechanism is needed to explain observations.

Institute for Climate and Atmospheric Science

Page 50: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Next steps

Remote sensing:

- Frequency of cloud: average the cloud occurrence from Calipso that are detached, at TTL heights, and close to balloon.

- Launch a balloon with humidity, particle counters, etc.

Institute for Climate and Atmospheric Science

Page 51: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Challenges

-Need an instrument to measure glassy particles.

-Understand aerosol spatial variations in the TTL and transport mechanisms.

-Assessing potential anthropogenic influences/indirect effects.

-Looking at warmer temperature glassy particles. Are they playing a role outside the tropics?

Institute for Climate and Atmospheric Science

Page 52: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

- Thank you -

Institute for Climate and Atmospheric Science

Page 53: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Institute for Climate and Atmospheric Science

Page 54: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Institute for Climate and Atmospheric Science

Page 55: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Institute for Climate and Atmospheric Science

Radiative heating rates Optical depth

Page 56: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Institute for Climate and Atmospheric Science

Forced by single waves: hom

Page 57: Institute for Climate and Atmospheric Science Balloons, waves and cirrus in the tropics Steven Dobbie Institute for Climate and Atmospheric Science University

Institute for Climate and Atmospheric Science

Radiative heating rates