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ECE 333 Green Electric Energy

ECE 333 Green Electric Energy. Lecture 12 The Solar Resource, continued Professor Tim O’Connell Department of Electrical and Computer Engineering. Announcements. Sections 4.3, 4.4, 4.5, 4.9

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ECE 333 Green Electric Energy

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  1. ECE 333 Green Electric Energy Lecture 12 The Solar Resource, continued Professor Tim O’Connell Department of Electrical andComputer Engineering

  2. Announcements • Sections 4.3, 4.4, 4.5, 4.9 • Today: Altitude Angle of the Sun at Solar Noon; Where is the Sun? Sun Path Diagrams for Shading; Clear-sky Direct Beam Radiation

  3. Solar Noon and Collector Tilt Solar noon – sun is directly over the local line of longitude Rule of thumb for the Northern Hemisphere: a South-facing collector tilted at an angle equal to the local latitude Figure 4.8 • On an equinox, during solar noon, the sun’s rays are perpendicular to the collector face

  4. Altitude Angle βN at Solar Noon Altitude angle at solar noon βN – angle between the sun and the local horizon Zenith – perpendicular axis at a site (4.7) Figure 4.9

  5. Solar Position at Any Time of Day Described in terms of altitude angle, β,and azimuth angle, ϕS ,of the sun β and ϕS depend on latitude, day number, and time of day Azimuth angle (ϕS ) convention Positive in the morning when Sun is in the East Negative in the evening when Sun is in the West reference in the Northern Hemisphere (for us) is true South Hours are referenced to solar noon

  6. Altitude Angle and Azimuth Angle (Solar noon) • Solar time – Noon occurs when the sun is over the local meridian (due South for us in the Northern Hemisphere above the tropics) Altitude Angle Azimuth Angle Figure 4.10

  7. Hour Angle • Hour angle H- the number of degrees the earth must rotate before sun will be over the local line of longitude • If we consider the earth to rotate at 15˚/hr, then • Examples: • At 11 AM solar time, H = +15˚ (the earth needs to rotate 1 more hour to reach solar noon) • At 2 PM solar time, H = -30˚ (4.10)

  8. Solar Coordinates • Calculate the position of the sun at any time of day on any day of the year: (4.8) (4.9) • Be careful! In Spring and Summer, the sun can be more than 90° from due South at sunset/sunrise: (4.11)

  9. Example: Where is the Sun? • Do Example 4.3 in text

  10. Sun Path Diagrams for Shading Analysis • Now we know how to locate the sun in the sky at any time • This can also help determine what sites will be in the shade at any time • Sketch the azimuth and altitude angles of trees, buildings, and other obstructions • Sections of the sun path diagram that are covered indicate times when the site will be in the shade • Shading of a portion of a solar panel could greatly reduce the output for the full panel (depending upon design)

  11. Sun Path Diagram for Shading Analysis: 40°N Latitude 90-40+23.45 = 73.45° (4.7) Solar noon Example 7.3 solution Figure 4.12

  12. Sun Path Diagram: 28°N Latitude 90-28+23.45 = 85.45° (4.7)

  13. Sun Path Diagram: 36°N Latitude 90-36+23.45 = 77.45° (4.7)

  14. Sun Path Diagram: 48°N Latitude 90-48+23.45 = 55.45° (4.7)

  15. Sun Path Diagram for Shading Analysis • Trees to the southeast, small building to the southwest • Can estimate the amount of energy lost to shading

  16. California Solar Shade Control Act • The shading of solar collectors has been an area of legal and legislative concern (e.g., a neighbor’s tree is blocking a solar panel) • California has the Solar Shade Control Act (1979) to address this issue • No new trees and shrubs can be placed on neighboring property that would cast a shadow greater than 10 percent of a collector absorption area between the hours of 10 am and 2 pm. • Exceptions are made if the tree is on designated timberland, or the tree provides passive cooling with net energy savings exceeding that of the shaded collector • Modified in 2008 to exclude systems designed to offset more than a building’s electricity demand

  17. The Guilty Trees were Subject to Court Ordered Pruning This case resulted in 2008 modificationto exclude existing trees (in this case theredwoods were planted before the panels were installed Source: NYTimes, 4/7/08

  18. How much sunlight reaches us? • We now know where the Sun is at any given time at any location on Earth • Based on this, how much solar insolation can we expect at a given site? • This will help us determine how much energy can be expected from a solar panel installation

  19. Clear Sky Direct-Beam Radiation • Direct beam radiation IBC – passes in a straight line through the atmosphere to the receiver • Diffuse radiationIDC – scattered by molecules in the atmosphere • Reflected radiationIRC – bounced off a surface near the reflector We’ll only focus on direct beam radiation in this class. Figure 4.19

  20. Extraterrestrial Solar InsolationI0 • I0 is the starting point for clear sky radiation calculations • I0 passes perpendicularly through an imaginary surface outside of the earth’s atmosphere Figure 4.20

  21. Extraterrestrial Solar InsolationI0 • I0varies with the Earth’s distance from the sun as well as sunspots and other solar activity • We will ignore sunspot effects • We can approximate I0 as: (4.19) SC = solar constant = 1.377 kW/m2 n = day number

  22. Extraterrestrial Solar InsolationI0 • Much of I0 is absorbed by various gases, scattered by dust, air molecules, water vapor, etc. • In one year, less than half of I0 reaches earth’s surface as a direct beam • On a sunny, clear day, beam radiation may exceed 70% of I0

  23. Attenuation of Incoming Radiation (4.20) • A = apparent extraterrestrial flux • k = optical depth • m = air mass ratio from (7.4) • IB = beam portion of the radiation that reaches the earth’s surface The A and k values are location dependent, varying with values such as dust and water vapor content

  24. Attenuation of Incoming Radiation • A and k values can be found from empirical data: 4.5 *This table is based on empirical data for a moderately dusty atmosphere with atmospheric water vapor content equal to the average monthly values in the US.

  25. Attenuation of Incoming Radiation • A and k values can also be found from a best fit equation based on measured data: (4.22) (4.23) *Best fit equations based on Table 4.5 data

  26. Example • Do Example 4.8 in text • Direct Beam Radiation at the Surface of the Earth.

  27. Solar Insolation on a Collecting Surface • Now that we know how to approximate the insolation reaching the Earth’s surface, we want to know how much will hit the face of a collector (solar panel) • The trick is to find the component of IB that is perpendicular to the collector

  28. Solar Insolation on a Collecting Surface • Direct-beam radiation on the collector face is just a function of the angle between the sun and the collecting surface (i.e., the incident angle q): (4.24) Special case: horizontal collector (panel flat on the ground)

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