Topic 2_Ch 5_"Radiation"
Topic 2: Energy and Radiation Balances
Chapter 5: Radiation
The Electromagnetic Spectrum
Fundamental Equations:
Speed of light: ( c = \lambda ,
u )Energy of radiation: ( Q = h ,
u ) or ( Q = \frac{h , c}{\lambda} )
Characteristics of Radiation:
All forms travel at the speed of light.
Capable of traveling through a vacuum.
Emitted by all entities based on their temperature.
Transports energy.
Emission of Radiation
Key Radiation Laws
Relationships between temperature and emitted radiation:
Planck’s law
Stefan–Boltzmann law
Wien’s law
Planck’s Curve
Represents blackbody radiation.
Rate of emission rises sharply with increasing wavelength, peaking at maximum emission wavelength ( \lambda_{max} ), then decreases gradually at longer wavelengths.
The Stefan–Boltzmann Law
The emission rate from a black body is proportional to the fourth power of its temperature: [ E = \epsilon , \sigma , T^4 ]
E: flux density (W·m⁻²)
( \epsilon ): emissivity (1 for black bodies)
( \sigma ): Stefan–Boltzmann constant (5.67 × 10⁻⁸ W·m⁻²·K⁻⁴)
Wien’s Law
Wavelength of maximum emission is inversely proportional to temperature.
Shorter wavelength = higher energy per photon (Planck's Law).
( \lambda_{max} \propto \frac{1}{T} )
Shortwave vs Longwave Radiation
Approximated black bodies:
Sun: Surface temperature ( T = 5800 K ); most emission between 0.15 and 3.0 μm (shortwave).
Earth: Surface temperature ( T = 288 K ); most emission between 3.0 and 100 μm (longwave).
Absorption, Reflection, and Transmission of Radiation
Interactions with surfaces:
Incident radiation can be absorbed, reflected, or transmitted.
Energy balance equation: ( a\lambda + \alpha\lambda + t\lambda = 1 ) or 100%.
a: absorption
α: reflection
t: transmission
Albedo: Measure of reflectivity.
Radiation in the Atmosphere: Scattering and Absorption
Effects of Radiation
Radiation absorbed in the atmosphere results in heating.
Radiation that is reflected or scattered can eventually reach the Earth's surface as diffuse radiation.
Direct beam of radiation reaches the surface when not absorbed or reflected.
Scattering
Scattering redirects radiation in various directions (Rayleigh and Mie scattering).
Absorption
Longwave radiation is more strongly absorbed than shortwave radiation.
Certain gases selectively absorb radiation:
Good absorbers of Sun’s radiation: Oxygen, ozone, water vapor.
Good absorbers of Earth’s radiation: Greenhouse gases (water vapor, CO₂, methane, etc.).
The Greenhouse Effect
Atmosphere allows solar radiation to pass but absorbs Earth’s longwave radiation.
Water vapor and CO₂ are primary absorbers.
Earth emits longwave radiation; some is absorbed by the atmosphere and re-emitted downwards.
Without the atmosphere, Earth would be 33 K cooler.
The Temperature Structure of the Atmosphere
Maximum temperature zones:
Upper thermosphere (absorption of 0.1–0.2 μm)
Upper stratosphere (absorption of 0.2–0.3 μm)
Lowest troposphere (heating at Earth’s surface).
Solar Radiation: Solar constant at the top of the atmosphere is 1361 W m⁻².
Sphericity and Sun Angles
Influences of Earth's Shape
Curvature effects:
Low latitudes: higher Sun angles.
High latitudes: lower Sun angles.
Seasonal variation in Sun intensity by latitude.
Sun Angle Definitions
Types:
Altitude angle
Zenith angle
Factors affecting Sun angle: latitude, longitude, time of year, time of day.
Seasonal Variations
Determinants of Seasons
Changes in:
Sun altitude above the horizon
Intensity of Sun's energy
Length of day
Earth’s Orbit: 23.5° axial tilt affects energy distribution.
Milankovitch Cycles
Eccentricity: 100,000-year cycle affects energy (±17 million km).
Tilt angle: Changes over 40,000 years (±1.2° total variation).
Tilt direction: Changes over 26,000 years affecting seasonality.
Conclusion: Reasons for Seasons
Functions of Earth’s physical characteristics and orbit:
Revolution around Sun.
Rotation on axis.
Axial tilt.
Axial parallelism.
Sphericity.
Annual march of the seasons.