Past and Future Climate of Thermospheric Density: Solar and Anthropogenic Influences

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Past and Future Climate of Thermospheric Density: Solar and Anthropogenic Influences Thermosphere energy balance Thermosphere climate from satellite drag Attribution of 2008 solar minimum behavior Scenarios for next 200 years Possible changes in the orbital debris population John Emmert, Judith Lean Space Science Division, Naval Research Lab Hugh Lewis Faculty of Engineering and the Environment, University of Southampton Acknowledgement: J. E. and J. L. were supported by the Chief of Naval Research

Roble, Geophys. Mon. 87, 1995 X-Rays Visible and IR Electric Currents and Energetic Particles IR Cooling Extreme UV 10-120 nm Far UV 120-200 nm Middle UV 200-300 nm Near UV 300-400 nm e Cooling Rates Troposphere Tides & Waves 2

SDO/AIA 30.4 nm Solar EUV Irradiance Variations Thermospheric Density Response ln Density Change 0-103 nm Irradiance (TIMED/SEE) 3

Thermospheric Composition and Mass Density O 2 N 2 O N He H Number Density (NRLMSISE-00) Diffusive Separation T ln ln ln m z 0 s ns ns0 dz T k z 0 B T z g z Total Mass Density (NRLMSISE-00) Solar Maximum ln ln T ln Hydrostatic Equilibrium M 0 0 0 1 g z T M k z0 T z B z M z dz Solar Minimum 4

www.esrl.noaa.gov CO 2 Cooling: A major driver of upper atmospheric changes CO 2 is increasing in the TROPOSPHERE and THERMOSPHERE Emmert et al., Nature Geoscience, 2012 Yue et al., GRL, 2015 5

Changes in Temperature and Density Cnossen, 2011 Modeled 1996-2008 Temperature Change Summary of Modeled and Observed Density Trends Qian et al., JGR, 2013 O 3 CH 4 /H 2 0 CO 2 All Modeled 1996-2008 Density Change Density O 3 CH 4 /H 2 0 CO 2 All Qian et al., JGR, 2013 6

Orbit-derived Thermospheric Density Data Description Derived from Global average mass density altitude profiles, 200-600 km Orbital drag on ~5000 objects Time covered 1967-2013 Temp. Resolution Absolute Accuracy Relative Accuracy 3-6 days ~10% ~2% Reference Emmert, JGR, 2015 a Rate of decay of an orbit is directly proportional to mass density. 2 3 d a Bv F dt a 400 km

Climate of Global Average Density (400 km) Solar EUV Irradiance Geomagnetic Activity F10.7 Intra-annual Oscillations Tropospheric CO 2 (ppm) 9 Emmert et al., JGR, 2014

Attribution of record-low thermospheric Densities Solar 400 km Geomagnetic Solar Activity In 2008 and 2009, lowest observed densities since beginning of space age Annual Variation Geomagnetic Activity CO 2 Residual 10 Emmert et al., JGR, 2014

Implicit Trends at Solar Minimum 1976.4 1986.7 1996.4 2008.8 Emmert, JGR, 2015 11

Solar Scenarios for Next 200 Years Scenario 1: Perpetual Grand Maximum (Cycle 18) Scenario 2: Gleissberg Minimum (Cycle 14) Scenario 3: Dalton Grand Minimum (Cycle 6) Scenario 4: Maunder + Gleissberg Minima 12

Solar Scenarios for Next 200 Years Tropospheric CO 2 (RCP 6.0) Solar Irradiance (F 10.7 ) Density at 400 km 13

CO 2 Scenarios for Next 200 Years Tropospheric CO 2 Roble & Dickinson, 1989 CO 2 Doubling Solar Irradiance (Scenario 2) Density at 400 km 14

The Orbital Debris Population NASA Debris Model, > 1 cm (~110,000) NASA Debris Model, > 10 cm (~7,500) Air Force Catalog (~11,500) Operational Satellites (~500) The Hazard: 18 cm 1.2 cm 15

Number of Objects > 10 cm The Orbital Debris Population Year NRC Debris Study, 2011 16

Top 10 worst fragmentations 17

UN Space Debris Mitigation Guidelines Limit debris released during normal operations. Minimize the potential for break-ups during operational phases. Limit the probability of accidental collision in orbit. Avoid intentional destruction and other harmful activities. Minimize potential for post-mission break-ups resulting from stored energy. Limit the long-term presence of spacecraft and launch vehicle orbital stages in the low Earth orbit (LEO) region after the end of their mission. are not enough to prevent debris growth: Atmospheric drag is currently the only way debris objects are removed from orbit. Active debris removal strategies are being researched. About 50 removals needed to prevent one collision. $1 $3 billion per year. 18

Debris Population Projections (No density trend) Average Evolution of 10 cm population 30% compliance w/mitigation guidelines 90% compliance 90% compliance with 5 removals p.a. Ensemble Variance, 30% compliance 19

Debris Population Projections (90% Compliance with Mitigation Guidelines) No Density Trend 8,082 objects With Density Trend 20

Summary Solar EUV irradiance is the dominant driver of thermospheric density variations on decadal and shorter time scales. Due to its dominant role as a cooling agent in upper atmospheric energy balance, CO 2 is a major driver of long-term change in the upper atmosphere. Satellite drag derived from orbital tracking data provides a long-term record of global thermospheric climate. Density at 400 km altitude is decreasing at rate of ~2% per decade, in quantitative agreement with model predictions of enhanced CO 2 cooling. Attribution of low density during the 2008 minimum is complicated by the fact that the major drivers (solar flux, geomagnetic activity, and CO2) all acted to produce negative inter-minima density trends. Long-term variations in solar output (e.g., Grand Maxima vs. Grand Minima), together with CO2 increases, would significantly alter thermospheric density, satellite drag, and the orbital debris population. Possible future states of the Sun and thermosphere should therefore be considered in planning debris remediation strategies. 21