Astroclimatology: How weather and climate affect astronomical viewing and site selection Dr. Edward Graham, University of the Highlands and Islands 1 Where is University of the Highlands and Islands (“UHI”)? Scotland !! 2 University of the Highlands and Islands (“UHI”) The Highlands and Islands E. Graham et al., 2010 3 University of the Highlands and Islands (“UHI”) E. Graham et al., 2010 4 Outline of my presentation today Two parts: 1) General Meteorology & Climatology BREAK / PAUSE 2) Application of above to Astronomy 5 Outline of my presentation today Two parts: 1) General Meteorology & Climatology BREAK / PAUSE 2) Application of above to Astronomy 6 Definition: Weather Weather is the state of the atmosphere at any one particular place at a particular time. Two separate places never have the exactly same weather, nor does the weather ever repeat itself Every moment of weather is unique in space and time 7 Definition: Climate • Is the « average » of the weather, over « reasonably » long period of time (e.g. 30 years) • Actual weather is usually chaotic, but is contained within certain boundaries, climate is the « average » 8 The scale of weather and climate systems • Weather and climate phenomena operate over huge temporal and spatial scales; • Spatially: 10-3 m (millimetres) to 106m (thousands of kilometres) • Temporally: 10-3 secs (milliseconds) to 108 secs (decades) 9 Is climate steady? Temperature (red) of last 20,000 years on Greenland ice cap 10 «Traditional» (deterministic) climatologists (until ~1980s) viewed climate as being reasonably steady. Present view is contrary to this: Climate itself may not be stable & there can be sudden « shifts » or «step-changes»… 10 Rate of current climate change… The rate of global climatic change is much faster than anything Earth has experienced in at least the last two millions years… (x 10 times faster) 11 Intergovernmental Panel on Climate Change (IPCC) scenarios for 21st century 12 Surface air temperature increase ~2090s 13 It’s not just a temperature increase…. An increase in Extremes too! 14 How does the Climate System work? Polar regions receive less solar radiation because: • • Ground surface area over which radiation is distributes gets larger towards poles Rays have a longer path length through atmosphere 15 How does the Climate System work? Result: • Unequal heating of the Earth’s surface by the sun, which varies according to day, season and latitude • The tilt of the Earth’s axis causes the seasons • The distribution of continents, mountains and oceans also play a key role • Atmosphere is a fluid, but 1000 times less dense than water • P = ρRT (Ideal gas equationl P=pressure, ρ=density, T=temperature, R=Universal gas constant) • Result is heat and moisture transfer towards the poles 16 The Earth’s Energy Balance On average, there’s 342 Wm-2 incident and outgoing radiation at the top of atmosphere, but clouds & aerosols alter the balance depending on location Hence there are energy transfers from equator to poles 17 Main methods of Energy Transfer on Earth The principal mechanisms driving this transfer of energy from the equator to the poles are the atmosphere and the oceans… Both transport about the same, despite sluggishly-moving ocean currents… Atmospheric Energy Transport: Wind H L Wind is just air moving from high pressure to low pressure (e.g. bicycle tyre) i.e. caused by a pressure gradient. As air gets warmer, it expands, becomes less dense and therefore pressure decreases. But there is the Coriolis Effect Helped by fact that air at the equator has greater relative angular velocity (40,000km per day) than air nearer the poles (0km/day). Wind and the Coriolis Effect The Coriolis Effect: H L Only for air that doesn’t “feel” the Earth’s rotation H L For air that “feels” the Earth’s rotation (Geostrophic balance) The resulting balance between the Coriolis Effect (due to the Earth’s rotation) and the Pressure-Gradient Force is “Geostropic balance” It means frictionless airflow is deflected by 90°…. Wind, the Coriolis Effect, and Friction H But differing amounts of surface friction (land, sea) result in a reduction in speed and a deflection reduced by 1030°… L Wind and the Coriolis Effect Air moving across latitudes in the Northern Hemisphere will swing to the right (clockwise). Air moving across latitudes in the Southern Hemisphere will swing to the left (anti-clockwise). The Jetstreams “Slopes” in pressure pattern then cause winds / the jetstream: -20C H L -10C 0C +10C Equator +20C North Pole 24 Differences in air temperature / air pressure cause the weather patterns: Differences in air temperature / air pressure cause the weather patterns: Latitudional (zonal) air circulation systems Rotation in weather systems - Lows Q: Why do low pressure turn anti-clockwise in the northern hemisphere? (and vice versa…) 1) 3) 2) L L L Rotation in weather systems - Lows Rotation in weather systems - Highs Q: And why do high pressures turn clockwise in the northern hemisphere? (and vice versa…) 1) 3) 2) H H H Rotation in weather systems - Highs General global pattern of surface air pressure The locations and intensities of these “highs” and “lows” vary with altitude. Geostropic flow around these weather systems is permitted for cases of no friction e.g. >1km above surface. But…. Non-geostropic flow can occur! • On small scales i.e. local or regional flow may not be geostrophic! H L • Especially true near mountains and coasts! • 1 deg latitude is roughly equivalent to 18km/h (11mph) difference in relative velocity! H L Non-Geostrophic Flow: The Sea Breeze Pressure difference forces air out to sea Warm air over land rises the sea-breeze moves onshore SEA LAND The logarithmic wind profile Where: u = windspeed (ms-1) u* = friction velocity (ms-1) k = Von Karman’s constant (0.4) z = height (m) d = zero-displacement height (m) z0 = roughness length (after Oke, 1976) = stability term The logarithmic wind profile “Free Atmosphere” (Geostrophic) ~300-1000m “Boundary Layer” (Non-Geostrophic) But turbulence can still form in “free atmosphere”: Windshear! “Free Atmosphere” (Geostrophic) Windshear ~300-1000m “Boundary Layer” (Non-Geostrophic) Turbulence in the “free atmosphere”: Instability “Free Atmosphere” (Geostrophic) Convection/bouyancy /instability “Boundary Layer” (Non-Geostrophic) Turbulence in the “free atmosphere”: Gravity Waves “Free Atmosphere” (Geostrophic) ~300-1000m “Boundary Layer” (Non-Geostrophic) Outline of my presentation today Two parts: 1) General Meteorology & Climatology BREAK / PAUSE 2) Application of above to Astronomy 40 Atmospheric Constraints on Astronomical Viewing 1. Clear skies / No Cloud 2. Stable Atmosphere / Little or no turbulence 3. Low Integrated Water Vapour (IWV) / Precipitable water (PWV) 4. Low night-time relative humidity (RH) 5. Gentle to moderate windspeeds, or less, throughout atmosphere 6. Moderate air temperatures, low variability 7. Low aerosol contamination 8. Infrequent or no severe weather (lightning, snow, hail) 9. Low light pollution Atmospheric Constraints on Astronomical Viewing 1. Clear skies / No Cloud 2. Stable Atmosphere / Little or no turbulence 3. Low Integrated Water Vapour (IWV) / Precipitable water (PWV) 4. Low night-time relative humidity (RH) 5. Gentle to moderate windspeeds, or less, throughout atmosphere 6. Moderate air temperatures, low variability 7. Low aerosol contamination 8. Infrequent or no severe weather (lightning, snow, hail) 9. Low light pollution 1. Cloud Cover: Clouds indicate ascending air It's cooler in the atmosphere as you go up, and cold air cannot hold as much water vapour as warm air. So, when air is forced to rise, the excess water vapour (gas) in the air condenses into liquid droplets. Three main processes which lift and cool air to form clouds 1) Sea / Sun heating (thermals) 2) Weather fronts (gentle) 3) Mountains Overall, the global upward movements of air are equally balanced by the downward movements, result is about 40-50% global cloudiness at any one time. 1. Cloud Cover: Astronomical Observation • Clouds occur on the local to synoptic (national/international) scales i.e. ~102 to ~105m spatial scale) and on temporal scales of 101 to 105 secs. • Vertical extent depends on forcing and stability • Local clouds occur especially daytime over mountain tops, and night-time in valleys (so good for astronomical observation) • Satellite (e.g. EUMETSAT) and climate model data (“reanalyses”) can be used to estimate cloud cover 1: Cloud Cover : Contrails 1: Cloud Cover : EUMETSAT satellite (1km nadir) 1: Cloud Cover : UK Met Office African model (12km) 1: Cloud Cover : FriOWL / Re-analyses data ERA40 reanalyses July total cloud cover (above 2,000m only) Atmospheric Constraints on Astronomical Viewing 1. Clear skies / No Cloud 2. Stable Atmosphere / Little or no turbulence 3. Low Integrated Water Vapour (IWV) / Precipitable water (PWV) 4. Low night-time relative humidity (RH) 5. Gentle to moderate windspeeds, or less, throughout atmosphere 6. Moderate air temperatures, low variability 7. Low aerosol contamination 8. Infrequent or no severe weather (lightning, snow, hail) 9. Low light pollution 2. A stable atmosphere with little turbulence • Covered by David / Aziz yesterday…. • Wobbling/scintillation of the stellar image is mostly due to the vertical temperature gradient i.e. when dT/dz is large - > unstable -> turbulence • But also mechanical turbulence due to mountains or obstacles • Descending air usually descends gently (unlike most ascending air, which ascends fast!) • It so happens that there are preferential zones zones of gently descending air around the globe… 2. A stable atmosphere with little turbulence Mean annual (1991-2000) ERA40 vertical velocities exceed 2.5 cm/sec (descent); these are indiciated by green / yellow/ red colours 2. A stable atmosphere with little turbulence H H H H H H H H ERA40 mid-to-upper tropospheric (775 to 200 hPa) vertical velocities in range 2.5 < > 5.0 cm /sec (i.e. gently subsiding air, turbulence less likely) Atmospheric Constraints on Astronomical Viewing 1. Clear skies / No Cloud 2. Stable Atmosphere / Little or no turbulence (~10-3 to ~105m) 3. Low Integrated Water Vapour (IWV) / Precipitable water (PWV) 4. Low night-time relative humidity (RH) 5. Gentle to moderate windspeeds, or less, throughout atmosphere 6. Moderate air temperatures, low variability 7. Low aerosol contamination 8. Infrequent or no severe weather (lightning, snow, hail) 9. Low light pollution 3. Low Integrated Water Vapour (IWV) / Precipitable water (PWV) IWV is extremely height dependent, due to exponential relationship of WV with temperature 3. Low Integrated Water Vapour (IWV) / Precipitable water (PWV) • • • • Water vapour is the principal absorbing gas from visible to millimeter wavelengths in the atmosphere Also increases the refractive index of air, causing phase distortions Decreases rapidly with vertical height; 2/3 less by a height of 2.5km Sarazin (2003) quotes: • < 5mm IWV is suitable for visible astronomy • <3mm for infra-red • <2mm for microwave Hence “High and Dry” sites are best…. Atacama, Rockies, Hawaii, Izana (Canarys), Morocco, Sutherland, African? 3. Low Integrated Water Vapour (IWV) / Precipitable water (PWV) 3. Low Integrated Water Vapour (IWV) / Precipitable water (PWV) 3. Low Integrated Water Vapour (IWV) / Precipitable water (PWV) Only locations where mean annual IWV at 700 hPa is less than 4 mm (yellow) and greater than 4 mm (blue) Atmospheric Constraints on Astronomical Viewing 1. Clear skies / No Cloud 2. Stable Atmosphere / Little or no turbulence (~10-3 to ~105m) 3. Low Integrated Water Vapour (IWV) / Precipitable water (PWV) 4. Low night-time relative humidity (RH) 5. Gentle to moderate windspeeds, or less, throughout atmosphere 6. Moderate air temperatures, low variability 7. Low aerosol contamination 8. Infrequent or no severe weather (lightning, snow, hail) 9. Low light pollution 4. Low night-time Relative Humidity (RH %) • RH is just the ratio of Vapour Pressure of Water Vapour ÷ Saturated Vapour Pressure at that same temperature 4. Low night-time Relative Humidity (RH %) • • • RH usually reaches a maximum during the night and around dawn (minima during afternoon) If RH = 100% -> dew / condensation / mist / frost Risk of dew/frost on mirror / lenses / optics Atmospheric Constraints on Astronomical Viewing 1. Clear skies / No Cloud 2. Stable Atmosphere / Little or no turbulence (~10-3 to ~105m) 3. Low Integrated Water Vapour (IWV) / Precipitable water (PWV) 4. Low night-time relative humidity (RH) 5. Gentle to moderate windspeeds, or less, throughout atmosphere 6. Moderate air temperatures, low variability 7. Low aerosol contamination 8. Infrequent or no severe weather (lightning, snow, hail) 9. Low light pollution 5. “Reasonably” low surface and jetstream windspeeds Sarazin (2004) states 2-9m/sec are ideal surface windspeeds for the VLT • <2m/sec -> no flushing of dome • >9 m/sec -> shake! Jetstream: Sarazin & Tokovinin (2002) show that the 200hPa jetstream is linearly related to the speed of turbulent structures on θ the stellar image Isoplanatic Angle (θ): the angle subtended to the telescope becomes smaller as height increases Atmospheric Constraints on Astronomical Viewing 1. Clear skies / No Cloud 2. Stable Atmosphere / Little or no turbulence (~10-3 to ~105m) 3. Low Integrated Water Vapour (IWV) / Precipitable water (PWV) 4. Low night-time relative humidity (RH) 5. Gentle to moderate windspeeds, or less, throughout atmosphere 6. Moderate air temperatures, low variability 7. Low aerosol contamination 8. Infrequent or no severe weather (lightning, snow, hail) 9. Low light pollution 6. Moderate Air Temperatures! • Differences between dome temperature and outside temperature can lead to “dome seeing” -> SALT is ventilated to keep dT/dx differences small! • Extreme cold /heat can put a strain on instrumentation, equipment and personnel ! Atmospheric Constraints on Astronomical Viewing 1. Clear skies / No Cloud 2. Stable Atmosphere / Little or no turbulence (~10-3 to ~105m) 3. Low Integrated Water Vapour (IWV) / Precipitable water (PWV) 4. Low night-time relative humidity (RH) 5. Gentle to moderate windspeeds, or less, throughout atmosphere 6. Moderate air temperatures, low variability 7. Low aerosol contamination 8. Infrequent or no severe weather (lightning, snow, hail) 9. Low light pollution 7. Low Aerosol Contamination • Aerosols (dust, biomass burning) contribute to atmospheric extinction • On-site wind-blown dust is a hazard as it degrades mirrors and optics rapidly (Giordano & Sarazin, 1994) • 22-years of TOMS aerosol data available on FriOWL Atmospheric Constraints on Astronomical Viewing 1. Clear skies / No Cloud 2. Stable Atmosphere / Little or no turbulence (~10-3 to ~105m) 3. Low Integrated Water Vapour (IWV) / Precipitable water (PWV) 4. Low night-time relative humidity (RH) 5. Gentle to moderate windspeeds, or less, throughout atmosphere 6. Moderate air temperatures, low variability 7. Low aerosol contamination 8. Infrequent or no severe weather (lightning, snow, hail) 9. Low light pollution & lots of others…. (infrastructure, culture, geology, accessibility, political issues, etc..) 8. Infrequent Severe Weather ! • Much greater exposure to lightning at the top of a mountain… • But the choice of a dry desert with few storms mitigates against chance of a lightning hit ! • Engineering needs to allow for specific loadings of snow ! Summary: There are links across a huge range of scales! Decadal cloudiness variability, Jetstream variations, Rossby waves (107m) Milliseconds, millimetres (CN2, CT2 CT2, seeing, r0, τ0) 1010 differences in scale Thank You (1017 difference in scales!) Hurricane Epsilon, 3 Dec 2005, NASA Spiral Galaxy, NGC 1232 21 Sep 1998, VLT Paranal (ESO) But 1017 times difference in scale!! 71