(Astro)Physics of the Earth system

Week

GEOS 3410

πŸͺ‘

Week Schedule

Tuesday

  1. Wrap-up Earth system
  2. States of matter and energy
  3. Electromagnetic radiation

Thursday

  1. EM, cont.
  2. Orbits & obital cycles
  3. The Sun & solar variability

Outside of class

  • Complete/self-grade quantitative skills packet & meet with me, by Friday
  • Lab 1 due 11:59 pm on Friday

States of matter


Sensible & latent heat

Electromagnetic Radiation

Electromagnetic Radiation

Behaves both like a …

  • wave: wavelength (λ), frequency (f)
  • particle: photons with discrete energy, E


\[\begin{aligned} \text{speed of light}~~ (m/s) \qquad c &= \lambda f \\ \text{energy}~~(J) \qquad E &= hf \\ \end{aligned}\] $$ \text{where} \qquad c = 3 \times 10^8~\text{m/s}, \qquad h = 6.67 \times 10^{-34}~\text{J~s} $$

Electromagnetic spectrum

Electromagnetic wavelengths you should know


Type/region λ range λmin (m) λmax (m)
Ultraviolet 10 – 400 nm 10−8 4×10-7
Visible 400 – 700 nm 4×10−7 7×10−7
Infrared 0.7 – 1000 µm 7 ×10−7 10-3

Behavior of light

Thermal radiation

An idealized scenario: the physical blackbody

Perfect absorber absorbs all incident radiation (α=0)
Ideal emitter emission depends only on temperature
Diffuse emitter emits evenly in all directions

Blackbody emission is a fuction of temperature

Total flux

(Stefan-Boltzmann law) \[\begin{aligned} F = \sigma T^4 \end{aligned} \]
… where $\sigma \approx 5.67 \times 10^{-8}~\text{W}~\text{m}^{-2}~\text{K}^{-4}$ (Stefan-Boltzmann constant)

Peak wavelength of emission

(Wien's displacement law) \[\begin{aligned} \lambda_{max} = \frac{b}{T} = \frac{0.0029~m\cdot K}{T} \approx \frac{3~mm\cdot K}{T} \end{aligned} \]

Why do we care about thermal emission?

Calculate the peak wavelength of blackbody emission for …

  1. The Sun: T = 5600 K ≈ 6000 K β˜€οΈ
  2. Saturn: T = 135 K ≈ 150 K πŸͺ
  3. Earth: T = 288 K ≈ 300 K 🌏
$$ \lambda_{max} = \frac{b}{T} \approx \frac{3~mm\cdot K}{T} $$

What happens to thermal emission when we warm an object?


Planck response

Spheres, radiation, and space

Spheres, radiation, and space

The solar radiant flux (W/m2) at a given distance d from the Sun's core is the solar luminosity L (W) spread over the area of a sphere.


How does incident flux $F$ scale with distance $d$ from the Sun?
$$F \propto \frac{1}{d^2}$$
Inverse square law

The solar constant

The solar flux at the top of Earth's atmosphere: $$G_{SC} = 1361~\text{W}~\text{m}^2$$ But, the average insolation of Earth's surface is ~340 W/m2
\[\begin{aligned} A_{disc} & = \pi r^2 \\ A_{sphere} & = 4 \pi r^2 \end{aligned}\]

Distribution of insolation

COMET / MetEd / UCAR, via Giannotti 2013

Orbits & orbital cycles

Planets (like Earth) orbit about their star and rotate about a spin axis.

Axial Tilt / Obliquity

Current obliquity ~ 23.5°

Tilt, Tropics & Circles

Obliquity and precession cycles

Obliquity: 41 kyr period, 22.1–24.5°
Axial Precession: 26 kyr period

Elliptical orbits have eccentricity


circle → e = 0      line → e = 1

Current e = 0.0167

Eccentricity cycles

Periods: 95 kyr, 124 kyr, 405 kyr
(mostly interactions with Jupiter and Saturn)

Milankovitch (orbital) cycles

Cycle Effect
Obliquity Seasonality – warmer/cooler winters and summers
Eccentricity Duration of seasons,
Insolation at perihelion & aphelion.
Precession Timing of seasons (relative to perihelion)

Milutin MilankoviΔ‡ crunched numbers on insolation (1910–1940)

Mean insolation at 65°N

Why do we care?

Quasiperiodic (periodic-ish) climate cycles

Spectral analysis of orbital records

Spectral analysis of climate records

All together now!

Cluster Reflection Time!

  1. Why can't orbital cycles account for modern climate change?
  2. Orbital cycles typically cause minor changes in insolation. So how can they drive glacial-interglacial cycles?
  3. Why do we care so much about the Northern Hemisphere?
  4. Glaciers (ice sheets) form from the accumulation of ice over many years. What will have a larger effect — colder winters or colder summers?
  5. Lingering questions.

The Sun

The Sun

Solar structure

  • Plasma (ionized gas)
  • Thermonuclear core
  • Outer convective surface
  • We see the photosphere, where the atmosphere becomes opaque

Solar magnetic field

The Sun is an ionized fluid!

Solar magnetic field

The Sun is an ionized fluid!
NASA / Wikimedia

Magnetic activity → sunspots

Magnetogram
Visible light intensity
Chromosphere
High magnetic activity → upwelling/downwelling → dark sunspots paired with brighter faculae (plages in chromosphere)

Solar cycle

~11-year cycle between low and high solar activity

Solar cycle over time

Solar irradiance varies by ~0.1% over the solar cycle

Sunspot variability and modern climate

Can we blame sunspots?

Lab this afternoon in MMS 273

Lab 1 due tomorrow (Friday) by 11:59pm

Next Week ()

  • Readings: Syllabus / Canvas
  • Meet with me on quantitative skills ASAP
  • Coming up: 🌎 Radiative 🌍 forcing 🌏