PHY2505S Atmospheric Radiation - PowerPoint PPT Presentation

1 / 22
About This Presentation
Title:

PHY2505S Atmospheric Radiation

Description:

Any theory to explain sunspots must also explain the butterfly effect of their ... Since most sunspot groups have, on average, about ten spots, this formula for ... – PowerPoint PPT presentation

Number of Views:49
Avg rating:3.0/5.0
Slides: 23
Provided by: Phys169
Category:

less

Transcript and Presenter's Notes

Title: PHY2505S Atmospheric Radiation


1
  • PHY2505S Atmospheric Radiation Remote
    SensingLecture 423/1/03
  • The Solar Radiation Source

2
The solar radiation source
  • The sun our nearest star
  • Geophysical parameters
  • Temperature structure composition
  • Photosphere, chronosphere, corona
  • Solar constant
  • Measurement
  • Diurnal latitudinal variation
  • Satellite measurements
  • Solar variability
  • Sunspots
  • Solar flares
  • Prominences
  • Magnetohydrodynamics
  • SOHO movies

3
The Sun our nearest star
  • Solar radius 695,990 km 432,470 mi 109
    Earth radii
  • Solar mass 1.989 1030 kg 4.376 1030 lb
    333,000 Earth masses
  • Solar luminosity (energy output of the Sun)
    3.846 x1033 erg/s 3.846 x 1026W
  • Surface temperature 5770 ºK 10,400 ºF
  • Surface density 2.07 10-7 g/cm3 1.6 x10-4 Air
    density
  • Surface composition 70 H, 28 He, 2 (C, N, O,
    ...) by mass
  • Central temperature 15,600,000 ºK 28,000,000
    ºF
  • Central density 150 g/cm3 8 Gold density
  • Central composition 35 H, 63 He, 2 (C, N, O,
    ...) by mass
  • Solar age 4.57 109 yr
  •  
  • From NASA Marshall Solar Physics
    http//science.msfc.nasa.gov/ssl/pad/solar/default
    .htm

4
The Sun our nearest star
  • 300,000 times closer to Earth than next
    nearest star
  • Energy nuclear fusion
  • 4 1H 2 e --gt 4He 2 neutrinos 6 photons
  • Producing 26 MeV 26 x 106 eV
  • 0.3 hydrogen mass converted to energy
  • 5 of solar mass converted to energy
  • Temperature in the core
  • Can estimate temperature in the core by
  • PROTON Thermal energy gravitational energy
  • 3/2kT GmpM/R, mp1.67 x 10-27 kg
  • T 2GmpM/3kR 1.56 x 107K

5
Temperature structure
  • Liou, Figure 2.1, 2.2

6
Photosphere, chronosphere, corona
  • Photosphere
  • Visible light from thin layer 400km thick,
    surface at temperature5800K, continuous
    radiation
  • UV continuum (1 of solar outpur)
  • Chronosphere corona
  • EUV, 120gt l gt 30nm
  • solar spectral lines

7
Solar absorption spectrum
http//www.coseti.org/highspec.htm
 
8
Solar constant
  • Calculate radiance in the direction of the sun
  • Flux normal to the beam is
  • FIsDW sT4 DW/p
  • 5.67e-8 x (5800)4 x 6.8e-5/ p
  • 4363/p
  • 1388.8K
  • This is the solar constant, S
  • How do we measure this?

9
Ground-based (long) method
  • Instrument measures IIoe-krz/cosq
  • Plot ln(I) ln (Io) krzsecq
  • Extrapolate back to secq0 to give Io
  • Integrate over l
  • Multiply by DW
  • Long method as takes
  • 2-3 hours of measurement
  • to calculate Io
  • Errors large zenith angle
  • non-homogeneity
  • multiple scattering
  • opaque regions of atmosphere

10
Variability due to orbit
F(t)S (ro/r)2 cos qo romean
distance qosolar zenith angle Eccentricity, e
0.017 Major axis ro(1e) Minor axis
ro(1-e) Variation ((1e)/(1-e))2 7 Solar
zenith angle cos qo sin y sin d cos y cos d
cos h Where y latitude d solar
declination h hour angle Solar noon, h0 Each
hour h15 degrees
Liou Figures 2.5 2.6
11
Diurnal variation
  • Insolation, Q
  • where angular velocity of the Earth, w dh/dt
  • H half solar day (radians)
  • cos H-tan y tan d
  • If y0 (equator) or d0 (equinoxes) then cos H 0
    and the length of the solar day is 12 hours
  • The latitude of the polar night H0 y90-d

12
Daily mean insolation (Q/24 hours)
Eqinoxes Solar declination, d
  • Liou, Figure 2.8

13
Satellite measurements of S
  • NIMBUS-7 16 Nov 78-13 Dec 93
  • Solar Maximum Mission (SMM) 16 Feb 80-01 Jun 89
  • Earth Radiation Budget Satellite (ERBS) 25 Oct
    84-21 Dec 94
  • NOAA-9 23 Jan 85-20 Dec 89 and 10 Oct 86-01
    Apr 87
  • Upper Atmospheric Research Satellite (UARS) 5 Oct
    91-30 Sep 94
  • Measured total solar irradiance, S, with
    radiometers equally sensitive across the full
    spectral range (EUV to far IR)
  • Typically 60 min orbit, with 35 min view of the
    sun

14
Satellite results
  • http//www.ngdc.noaa.gov/stp/SOLAR/IRRADIANCE/i
    rrad.html
  • Offsets between instruments
  • Solar maxima, minima
  • Smallscale variability

15
Offsets between instruments
  • . SSM/UARS Active Cavity Radiometer
    Irradiance Monitor (ACRIM)
  • The principle of measuring total solar irradiance
    is that the heating effect of irradiant flux on a
    detector is compared with that of electrical
    power dissipated in a heating element in intimate
    thermal contact with the detector. An accurate
    knowledge of the effective absorptance of the
    detector for the irradiant flux, the area over
    which the detector is illuminated and the
    electrical heating power facilitates the accurate
    measurement of irradiant fluxes on an absolute
    basis in the International System of Units. The
    total solar irradiance data, expressed in Watt
    per square meter at the instrument, are
    calculated based on the equation
  • S K(Pref-Pobs)E
  • where S is the calculated irradiance, Pref and
    Pobs are the cavity electrical heating powers
    during the reference and observational phase of
    the measurements. K is the standard detector
    constant of proportionality which contains
    instrument parameters, such as the area of the
    primary aperture, effective cavity absorptance
    for solar irradiance, cavity reflectance for
    solar irradiance, and reflectance of solar
    radiation by the cavity field of view. E
    summarizes small terms due to small departures
    from instrument equilibrium.
  • Corrections for temperature dependence, solar
    viewing angle, Sun-satellite distance and
    relative velocity, and sensor degradation
  • From http//www.ngdc.noaa.gov/stp/SOLAR/IRRADIANCE
    /uars.html

16
Sunspots
  • Sunspots have been observed for centuries.
  • Early question was whether the dark blobs seen
    on the visible disc of the sun were planets
    passing across the disc or clouds. Galileos
    1610 observations showed a foreshortening of the
    images over some days from which he interpreted
    correctly that the blobs must be on the surface
    of the sun

http//www.exploratorium.edu/sunspots http//scien
ce.msfc.nasa.gov/ssl/pad/solar/
17
Sunspot cycle
  • The sunspot number has been
    seen to vary with a period from maximim to
    maximum of 11 years.
  • Any theory to explain sunspots must also explain
    the butterfly effect of their motion

The "sunspot number" the sum of the number of
individual sunspots and ten times the number of
groups. Since most sunspot groups have, on
average, about ten spots, this formula for
counting sunspots gives reliable numbers even
when the observing conditions are less than ideal
and small spots are hard to see.
18
..And other observed variability in the sun
The total solar output (solar
constant ) variation is found to correlate with
the sunspot maximum and minimum
cycle Solar activity is also seen in the
form of prominences, flares and changes to the
solar wind
19
Solar and Heliospheric Observatoryhttp//sohowww.
nascom.nasa.gov/L1 point - an uninterrupted view
of the sun
20
Prominences and flares
  • Prominences huge clouds of relatively cool,
    dense plasma suspended in the Sun's hot, tenuous
    corona
  • Flares enormous explosions in the surface of the
    sun, ejecting energy and matter post flare
    loops are shown above http//science.msfc.nasa.gov
    /ssl/pad/solar/loops.htm

21
Magnetohydrodynamics
  • Solar activity is thought to be due to
    interaction between the suns magnetic field,
    solar rotation rate, and convection

22
SOHO movies
Write a Comment
User Comments (0)
About PowerShow.com