Successfully reported this slideshow.
We use your LinkedIn profile and activity data to personalize ads and to show you more relevant ads. You can change your ad preferences anytime.

Solar Radiation Geometry

26,990 views

Published on

Published in: Technology, Business
  • Mam can you send the presentation to me on my mail it will help me
       Reply 
    Are you sure you want to  Yes  No
    Your message goes here
  • please send this presentation on aachrekarharsh@gmail.com
       Reply 
    Are you sure you want to  Yes  No
    Your message goes here
  • Resp mam, presentation is awsome, kindly mail on patil.amol2015@rediffmail.com
       Reply 
    Are you sure you want to  Yes  No
    Your message goes here
  • nice ppt madam. I would greatly appreciate if you send this ppt to ravikishorgandi@gmail.com. thank you very much for making such a beautiful ppt
       Reply 
    Are you sure you want to  Yes  No
    Your message goes here
  • very good presentation please send it to me in this mail
       Reply 
    Are you sure you want to  Yes  No
    Your message goes here

Solar Radiation Geometry

  1. 1. SOLAR RADIATION GEOMETRY -VANITA THAKKAR ASSOCIATE PROFESSOR, MECHANICAL ENGINEERING DEPARTMENT, BABARIA INSTITUTE OF TECHNOLOGY, VARNAMA, VADODARA.
  2. 2. SOLAR ENERGY • Sun is the basic source of Energy for Earth. • Solar Energy is available in the form of Electromagnetic Radiations. • Sun is a large sphere of very hot gases, heat being generated by the various fusion reactions in it. • Diameter of Sun = 1.39 x 106 km. • Diameter of Earth = 1.27 x 104 km. • Sun subtends an angle of only 32’ at Earth’s surface (because of large distance between them.) 2 VANITA N. THAKKAR BIT, VARNAMA
  3. 3. SOLAR ENERGY • The direct / beam radiation received from the Sun on the earth is almost parallel. • Brightness of the Sun varies from its centre to its edge, however, for engineering calculations, it is assumed to be uniform over the entire solar disc. 3 VANITA N. THAKKAR BIT, VARNAMA
  4. 4. SOLAR ENERGY • The sun generates an enormous amount of energy - approximately 1.1 x 1020 kilowatt- hours every second. (A kilowatt-hour is the amount of energy needed to power a 100 watt light bulb for ten hours.) 4 VANITA N. THAKKAR BIT, VARNAMA
  5. 5. SOLAR ENERGY ON EARTH • The earth’s outer atmosphere intercepts about one two-billionth of the energy generated by the sun, or about 1500 quadrillion (1.5 x 1018 ) kilowatt-hours per year. • Due to Reflection, Scattering, and Absorption by gases and aerosols in the atmosphere, however, only 47% of this, or approximately 700 quadrillion (7 x 1017 ) kilowatt-hours per year, reaches the surface of the earth. 5VANITA N. THAKKAR BIT, VARNAMA
  6. 6. SOLAR ENERGY ON EARTH (contd.) • In the earth’s atmosphere, solar radiation is received : – directly (Direct Radiation) and – by diffusion in air, dust, water, etc., contained in the atmosphere (Diffuse Radiation). • Global radiation = Direct Radiation + Diffuse Radiation. • The amount of incident energy per unit area and day depends on a number of factors, e.g. : – Solar Radiation Geometry, which includes Solar Angles, Locational or Geographical factors and Season / Time of the year. – Local climate. – Inclination of the collecting surface in the direction of the sun. 6VANITA N. THAKKAR BIT, VARNAMA
  7. 7. EARTH’S ROTATION • The term Earth’s rotation refers to the spinning of Earth on its axis. • Due to rotation, the Earth's surface moves at the equator at a speed of about 467 m per second or slightly over 1675 km per hour. • One rotation takes exactly twenty- four hours and is called a mean solar day. • The Earth’s rotation is responsible for the daily cycles of day and night – i.e. at any moment in time, one half of the Earth is in sunlight, while the other half is in darkness. • The edge dividing the daylight from night is called the circle of illumination. • The Earth’s rotation also creates the apparent movement of the Sun across the horizon. A line that bisects areas on the Earth receiving sunlight and those areas in darkness. Cuts the spherical Earth into lighted and dark halves. 7 VANITA N. THAKKAR BIT, VARNAMA
  8. 8. EARTH’S ROTATION (contd.) • Looking down at the Earth's North Pole from space one would see that the direction of rotation is counter-clockwise. • Looking down at the Earth's South Pole from space one would see that the direction of rotation is clockwise. 8VANITA N. THAKKAR BIT, VARNAMA
  9. 9. EARTH REVOLUTION • The orbit of the Earth around the Sun is called an Earth revolution. • This celestial motion takes 365.26 days to complete one cycle. • Earth's orbit around the Sun is not circular, but oval or elliptical. • An elliptical orbit causes the Earth's distance from the Sun to vary over a year. Yet, this phenomenon is not responsible for the Earth’s seasons ! • This variation in the distance from the Sun causes the amount of solar radiation received by the Earth to annually vary by about 6%. 9VANITA N. THAKKAR BIT, VARNAMA
  10. 10. POSITIONS IN EARTH’S REVOLUTION Positions in the Earth’s revolution : On January 3, Perihelion, Earth is closest to the Sun (147.3 million km). On July 4, Aphelion, Earth is farthest from the Sun (152.1 million km). Average distance of Earth from the Sun over one-year period is ~ 149.6 million km, i. e. 1.496 x 108 km. 10 VANITA N. THAKKAR BIT, VARNAMA
  11. 11. SOLAR CONSTANT • Measurements indicate that the Energy Flux (rate of energy transfer through a unit area) received from Sun outside the Earth’s atmosphere is essentially constant : • SOLAR CONSTANT (ISC) : The rate at which Energy is received from the Sun on a unit area perpendicular to the rays of Sun, at a mean distance of the Earth from the Sun (~ 1.496 x 108 km). ISC = 1367 W/m2 • The solar constant includes all types of solar radiation, not just the visible light. 11 VANITA N. THAKKAR BIT, VARNAMA
  12. 12. VARIATION IN EXTRA-TERRESTRIAL FLUX • Due to variation in Earth-Sun distance throughout the year, the Extra- terrestrial Flux varies, which can be calculated from the equation : ISC’ = ISC [1 + 0.033 cos (360n/365)], Where, n = the number of day of the year. 12VANITA N. THAKKAR BIT, VARNAMA
  13. 13. TILT OF EARTH’S AXIS • The ecliptic plane can be defined as a two-dimensional flat surface that geometrically intersects the Earth's orbital path around the Sun. • On this plane, the Earth's axis is not at right angles to this surface, but inclined at an angle of about 23.5° from the perpendicular. 13VANITA N. THAKKAR BIT, VARNAMA
  14. 14. SOLISTICE AND EQUINOX Figure shows a side view of the Earth in its orbit about the Sun on four important dates: June solstice, September equinox, December solstice, and March equinox. Angle of the Earth's axis in relation to the Ecliptic Plane and the North Star on these four dates remains unchanged. 14 VANITA N. THAKKAR BIT, VARNAMA
  15. 15. SOLISTICE AND EQUINOX (contd.) • Yet, the relative position of the Earth's axis to the Sun does change during this cycle. • This is responsible for the annual changes in the height of the Sun above the horizon. • It also causes the seasons, by controlling the intensity and duration of sunlight received by locations on the Earth. 15 VANITA N. THAKKAR BIT, VARNAMA
  16. 16. SOLISTICE AND EQUINOX (contd.) • In an overhead view of the same phenomenon, one can see how the circle of illumination changes its position on the Earth’s surface. • During the two equinoxes, the circle of illumination cuts through North Pole and South Pole. • On the June solstice, the circle of illumination is tangent to the Arctic Circle (66.5° N) and the region above this latitude receives 24 hours of daylight. The Arctic Circle is in 24 hours of darkness during the December solstice. 16VANITA N. THAKKAR BIT, VARNAMA
  17. 17. SOLISTICE • On June 21 or 22 (also called the summer solstice in Northern Hemisphere) Earth is positioned in its orbit so that North Pole is leaning 23.5° toward the Sun : All locations north of the equator have day lengths greater than twelve hours, while all locations south of the equator have day lengths less than twelve hours. • On December 21 or 22 (also called the winter solstice in Northern Hemisphere), Earth is positioned so that South Pole is leaning 23.5 degrees toward the Sun : All locations north of the equator have day lengths less than twelve hours, while all locations south of the equator have day lengths exceeding twelve hours. 17VANITA N. THAKKAR BIT, VARNAMA
  18. 18. EQUINOX • On September 22 or 23, also called the autumnal equinox in the Northern Hemisphere, neither pole is tilted toward or away from the Sun. • In the Northern Hemisphere, March 20 or 21 marks the arrival of the vernal equinox or spring when once again the poles are not tilted toward or away from the Sun. • Day lengths on both of these days, regardless of latitude, are exactly 12 hours. 18 VANITA N. THAKKAR BIT, VARNAMA
  19. 19. EARTH’S REVOLUTION 19VANITA N. THAKKAR BIT, VARNAMA
  20. 20. SPECTRAL DISTRIBUTION OF SOLAR RADIATION Solar Radiation spectrum is close to that of a black body with a temperature of about 5,800 K. About half that lies in the visible short- wave part of and the other half mostly in near-infrared part. Some also lies in the ultraviolet part of the spectrum. Spectrum of electromagnetic radiation striking Earth's atmosphere : 100 to 106 nm, divided into five regions : 20 VANITA N. THAKKAR BIT, VARNAMA
  21. 21. SPECTRAL DISTRIBUTION OF SOLAR RADIATION (contd.) Ultraviolet C (UVC) : 100 to 280 nm. Radiation Frequency > violet light Frequency (so, invisible to human eye). Mostly absorbed by Lithosphere. Ultraviolet B (UVB) : 280 to 315 nm. Mostly absorbed by atmosphere; Along with UVC, responsible for photochemical reaction leading to production of Ozone layer. Ultraviolet A (UVA) : 315 to 400 nm. Considered less damaging to the DNA Visible range or light : 400 to 700 nm. Infrared range : 700 nm to 106 nm. An important part of the electromagnetic radiation reaching Earth. Divided into three types : Infrared-A: 700 nm to 1,400 nm Infrared-B: 1,400 nm to 3,000 nm Infrared-C: 3,000 nm to 1 mm. 21 VANITA N. THAKKAR BIT, VARNAMA
  22. 22. SPECTRAL DISTRIBUTION OF SOLAR RADIATION (contd.) • Maximum value of Solar Radiation Intensity = 2074 W/m2 occurs at 0.48mm wavelength. • 99% of solar radiation is obtained upto a wavelength of 4mm. Wave length (mm) 0.00- 0.38 0.38- 0.78 0.78- 4.0 Approx. energy (W/m2) 95 640 618 Approx. % of total energy 7% 47.3 % 45.7 % 22 VANITA N. THAKKAR BIT, VARNAMA
  23. 23. SOLAR RADIATION ON EARTH’S SURFACE • Solar radiation reaching the Earth’s surface differs in amount and character from Extraterrestrial Radiation. • Part of the radiation is reflected back, especially by clouds. • Some part of it is absorbed by molecules in air such as – – O2 and O3 (ozone) absorb nearly all UV radiations. – Water vapour and CO2 absorb some energy in infrared range. • Some part of it is scattered by droplets in clouds and dust particles. 23 VANITA N. THAKKAR BIT, VARNAMA
  24. 24. DIRECT AND DIFFUSE RADIATION Direct / Beam Radiation : Solar radiation that does not get absorbed or scattered, but reaches the ground directly from the Sun. It produces shadow when interrupted by an opaque object. Diffuse Radiation : Solar radiation received after its direction has been changed by reflection and scattering in the atmosphere. 24VANITA N. THAKKAR BIT, VARNAMA
  25. 25. ATTENUATION OF SOLAR RADIATION 25VANITA N. THAKKAR BIT, VARNAMA
  26. 26. SOLAR RADIATION GEOMETRY Angles useful in Solar Radiation Analysis : 1. Latitude of location (fl). 2. Declination (d). 3. Hour Angle (w). 4. Altitude Angle (a). 5. Zenith Angle (qz). 6. Solar Azimuth angle (gs). 7. Slope (s). 26VANITA N. THAKKAR BIT, VARNAMA
  27. 27. LATITUDE ANGLE (fl) Latitude (fl) Latitude of location (fl) : Angle made by radial line joining the location to the centre of the Earth and the projection of that line on the Equatorial plane. It is the angular distance north or south of equator measured from centre of Earth. It varies from 0o at equator to 90o at the poles. 27 VANITA N. THAKKAR BIT, VARNAMA
  28. 28. LATITUDE ANGLE (fl) (contd.) Latitude along with the longitude indicates the position of any point on earth. 28 VANITA N. THAKKAR BIT, VARNAMA
  29. 29. DECLINATION (d) On Equinoxes, Declination = 0 It is given by : Declination Angle (d)Declination (d) : Angular distance of the sun’s rays north or south of the equator. It is the angle between a line extending from the centre of Sun to centre of Earth and the projection of this line upon Earth’s Equatorial Plane. It is due to tilt of Earth’s axis and it varies between 23.5o (Summer Solstice : June 22) to -23.5o (Winter Solstice : December 22). 29 VANITA N. THAKKAR BIT, VARNAMA
  30. 30. DECLINATION (d) (contd.) 30 VANITA N. THAKKAR BIT, VARNAMA
  31. 31. DECLINATION (d) (contd.) Declination Angle (d) 31 VANITA N. THAKKAR BIT, VARNAMA
  32. 32. REMEMBER : EARTH’S REVOLUTION Changes in DECLINATION shown by Changes in the Red Line 32 VANITA N. THAKKAR BIT, VARNAMA
  33. 33. HOUR ANGLE (w) Hour Angle (w) Hour Angle (w) : The angle through which the earth must turn to bring the Meridian of a point directly in line with the Sun’s rays. It is a measure of the time of the day with respect to solar noon. At noon, w = 0. w= 15o per hour. It is measured from noon, based on the Local Solar Time (LST), +ve before noon and -ve during afternoon. Solar noon occurs when the sun is at the highest point in the sky & w is symmetric with respect to solar noon. 33 VANITA N. THAKKAR BIT, VARNAMA
  34. 34. LOCAL SOLAR TIME Solar Time can be obtained from Standard Time observed on a clock by applying Two Corrections : 1. Due to difference in Longitude between a location and the meridian on which the standard Time is based : Has a magnitude of 4 minutes for every degree difference in Longitude. 2. Due to Equation of Time : As Earth’s orbit and rate of rotation are subject to small perturbations. 34VANITA N. THAKKAR BIT, VARNAMA
  35. 35. LOCAL SOLAR TIME (contd.) 35 VANITA N. THAKKAR BIT, VARNAMA
  36. 36. LOCAL SOLAR TIME (contd.) EQUATION OF TIME - GRAPH 36 VANITA N. THAKKAR BIT, VARNAMA
  37. 37. LST = Standard Time ± 4 (Standard Time Longitude – Longitude of Location) + (Equation of Time Correction) The negative sign is applicable for Eastern Hemisphere. Important Note : Hour Angle, w = 15 (12 - LST) LOCAL SOLAR TIME (LST) (contd.) 37VANITA N. THAKKAR BIT, VARNAMA
  38. 38. PROBLEM – 1 : Determine Hour Angle for : 09:00 AM, 11:00 AM, 02:00 PM, 04:30 PM SOLUTION : Hour Angle, w = 15 (12 - LST) 09:00 AM : w = 15(12 – 9) = 45o 11:00 AM : w = 15(12 – 11) = 15o 02:00 PM : w = 15(12 – 14) = -30o 04:30 AM : w = 15(12 – 16.5) = -67.5o 38 VANITA N. THAKKAR BIT, VARNAMA
  39. 39. PROBLEM – 2 : Determine the LST and Declination at a location latitude 23o15’ N, longitude 77o30’ E at 12.30 IST on June 20. EOT correction = -(1’ 02”). Standard Time Longitude for IST = 82.5o. 39VANITA N. THAKKAR BIT, VARNAMA
  40. 40. PROBLEM – 3 : Determine the LST and Declination at a location latitude 23o15’ N, longitude 67o30’ E at 02.30pm IST on October 02. EOT correction = (9’ 02”). Standard Time Longitude for IST = 82.5o. 40VANITA N. THAKKAR BIT, VARNAMA
  41. 41. ALTITUDE ANGLE (a) Altitude Angle or Solar Altitude (a) : Vertical angle between the projection of Sun’s rays on the horizontal plane on Earth’s surface and the direction of Sun’s ray. The altitude angle a is maximum at solar noon. Altitude (a) 41 VANITA N. THAKKAR BIT, VARNAMA
  42. 42. ZENITH ANGLE (qz) Zenith Angle (qz) : Complimentary angle of Solar Altitude Angle, i.e. Vertical angle between Sun’s rays and a line perpendicular to the horizontal plane though the point, i.e. Angle between the beam from the sun and the vertical. qz = p/2 - a Zenith Angle (qz) 42 VANITA N. THAKKAR BIT, VARNAMA
  43. 43. SOLAR AZIMUTH ANGLE (gs) Solar Azimuth Angle (gs) : Solar Angle in degrees along the horizon east or west of North. It is a horizontal angle measured from North to horizontal projection of sun’s rays. It is consider +ve west-wise. Solar Azimuth Angle (gs) 43 VANITA N. THAKKAR BIT, VARNAMA
  44. 44. RELATION BETWEEN BASIC SOLAR ANGLES Basic Solar Angles : 1. Latitude of location (fl or l). 2. Declination (d or d). 3. Hour Angle (w or h). Derived Solar Angles : 1. Altitude Angle (a). 2. Zenith Angle (qz). 3. Solar Azimuth angle (gs). cos qz = cos f cos w cos d + sin f sin d = sin a …… (as qz = p/2 - a) cos gs = sec a (cos f sin d– cos d sin f cos w) sin gs = sec a cos d sin w 44VANITA N. THAKKAR BIT, VARNAMA
  45. 45. SLOPE (s) Slope (s) : Angle made by the plane surface with the horizontal. It is : +ve : for surfaces slopping towards South -ve : for surfaces slopping towards North. Slope (s) 45VANITA N. THAKKAR BIT, VARNAMA
  46. 46. ANGLE OF INCIDENCE (q) When Tilted Surfaces are involved : ANGLE OF INCIDENCE (q) : Angle between Sun rays and normal to surface under consideration. 46 VANITA N. THAKKAR BIT, VARNAMA
  47. 47. SURFACE AZIMUTH ANGLE (g) For Tilted Surfaces : SURFACE AZIMUTH ANGLE (g) : Angle of deviation of the normal to the surface from the local meridian, It is angle between the normal to the surface and south. For south-facing surface, g = 0. For west-facing surface, g = 90o and so on. East-ward : +ve, West-ward : -ve. SURFACE AZIMUTH ANGLE (g) 47 VANITA N. THAKKAR BIT, VARNAMA
  48. 48. GENERAL EQUATION FOR ANGLE OF INCIDENCE (q): cos q = sin fl (sin d cos s + cos d cos g cos w sin s) + cos fl (cos d cos w cos s – sin d cos g sin s) + cos d sin g sin w sin s ……………. (i) LatitudeDeclination Surface Azimuth Angle Hour Angle Slope 48 VANITA N. THAKKAR BIT, VARNAMA
  49. 49. ANGLE OF INCIDENCE (q) FOR VERTICAL SURFACES : For Vertical Surfaces : Slope, s = 90o So, from Equation (i) : cos q = sin fl (sin d cos s + cos d cos g cos w sin s) + cos fl (cos d cos w cos s – sin d cos g sin s) + cos d sin g sin w sin s => cos q = sin fl cos d cos g cos w – cos fl sin d cos g + cos d sin g sin w …….. (ii) = 0 = 1 49 VANITA N. THAKKAR BIT, VARNAMA
  50. 50. ANGLE OF INCIDENCE (q) FOR HORIZONTAL SURFACES : For Horizontal Surfaces : Slope, s = 0o, Zenith Angle qz = q So, from Equation (i) : cos q = sin fl (sin d cos s + cos d cos g cos w sin s) + cos fl (cos d cos w cos s – sin d cos g sin s) + cos d sin g sin w sin s Hence, cos q = sin fl sin d + cos fl cos d cos w = sin a ……….. (iii) i.e. cos q = cos qz = sin a = 1 = 0 50 VANITA N. THAKKAR BIT, VARNAMA
  51. 51. ANGLE OF INCIDENCE (q) FOR SURFACES FACING SOUTH : For Surfaces facing due south : Surface Azimuth Angle, g = 0o, So, from Equation (i) : cos q = sin fl (sin d cos s + cos d cos g cos w sin s) + cos fl (cos d cos w cos s – sin d cos g sin s) + cos d sin g sin w sin s Hence, cos q = sin fl (sin d cos s + cos d cos w sin s) + cos fl (cos d cos w cos s – sin d sin s) … (iv) =>cos q = sin d sin (f – s) + cos d cos w cos (f – s) = 1 = 0 51 VANITA N. THAKKAR BIT, VARNAMA
  52. 52. ANGLE OF INCIDENCE (q) FOR VERTICAL SURFACES FACING SOUTH : For Vertical Surfaces facing due south : Surface Azimuth Angle, g = 0o, slope, s = 90o So, from Equation (i) : cos q = sin fl (sin d cos s + cos d cos g cos w sin s) + cos fl (cos d cos w cos s – sin d cos g sins ) + cos d sin g sin w sin s Hence, cos q = sin fl cos d cos w + cos fl sin d ………….. (v) = 1 = 0 52 VANITA N. THAKKAR BIT, VARNAMA
  53. 53. DAY LENGTH At the time of sunrise or sunset, the Zenith angle, fz = 90o. Substituting this in equation (iii) obtained earlier : cos q = sin fl sin d + cos fl cos d cos w = sin a (= 0) Sun Rise Hour Angle (ws) : cos ws = -(sin f sin d) / (cos f cos d) cos ws = - (tan f tan d)  ws = cos-1(- tan f tan d) ……….. (vi) 53 VANITA N. THAKKAR BIT, VARNAMA
  54. 54. DAY LENGTH (contd.) Since, ws = 15o per hour, Day Length (in hours) = td = (2 ws / 15) i.e. td = (2 / 15) cos-1(- tan f tan d) Thus, day length is a function of latitude f and solar declination d. 54VANITA N. THAKKAR BIT, VARNAMA
  55. 55. THANKS !! Contact : vanitaa.thakkar@gmail.com 55VANITA N. THAKKAR BIT, VARNAMA

×