4. energy meteorology (eee 483)

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Md. Rashedul Haque Adjunct Faculty, EEE Energy Meteorology –EE483 10/28/2015

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Page 1: 4. Energy Meteorology (EEE 483)

Md. Rashedul HaqueAdjunct Faculty, EEE

Energy Meteorology –EE483

10/28/2015

Page 2: 4. Energy Meteorology (EEE 483)

10/28/2015

Black Body: An ideal black body absorbs all incident electromagnetic radiation fall on it and also emits e-m radiation of all frequencies when heated.

Radiations Laws: Plank’s Black Body Radiation Law: The energy radiated

away from a blackbody at temperature T and wavelength λcan be obtained from Planks Black body radiation law:

Basic Law

Page 3: 4. Energy Meteorology (EEE 483)

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Wien’s displacement law : The relationship between the wavelength of a black body’s maximum emission λm and the corresponding absolute temperature is given by:

Stefan-Boltzmann law: Integration of Planck’s function over the entire wavelength domain leads to the fundamental Stefan-Boltzmann law, which gives the total radiant flux density emitted by a blackbody at temperature T (emitted radiation per unit time and area):

Basic Law

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The is the largest member of the solar system, having a diameter of 1.39 x 109m.

An average distance from earth is 1.495 x 1011m. The core temperature estimated between 8x106 to 40x106

ok. The Sun is a natural fusion reactor. Several fusion reaction

have been suggested to be source of the energy radiant by the sun. The most important of them is four hydrogen atoms combine to form helium, the difference of the mass have been converted to energy.

The Sun as a Source of Energy

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The Diameter of the Earth about 1.275 x 107 m. Its axis is inclined at an angle of 23.5o. The Earth reflects about 30% of sunlight that fall on it.

The Earth

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Sun, Earth Radiation Spectrum

Page 7: 4. Energy Meteorology (EEE 483)

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Absorption Scattering Beam Radiation Diffuse Radiation Global Radiation Air mass

Depletion of Solar Radiation

Page 8: 4. Energy Meteorology (EEE 483)

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Extraterrestrial and Terrestrial Radiation

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Spectral Energy Distribution of Solar Radiation

Page 10: 4. Energy Meteorology (EEE 483)

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Pyranometer

Pyrheliometer

Measurement of Solar Radiation

Page 11: 4. Energy Meteorology (EEE 483)

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For calculating the solar radiation and design the solar device, we have to know the Sun’s path in the sky on the various day in a year at a particular place.

Position of Sun

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It is the angle between sun’s ray incident on the plane surface(collector) and the normal to that surface.

Its depends on Geographical location (Latitude), ф Time of the year (Declination angle), δ Time of the day (Hour angle), ω Orientation of the plane (slope(β),

Surface azimuth (γ))

Θi=f(ф,δ,ω,β,γ)

Angle of incidence (θi)

Page 13: 4. Energy Meteorology (EEE 483)

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Solar Radiation Geometry

Latitude (Angle of Latitude), ф: The latitude of a location on the earth’s surface is the angle made by a radial line joining the given location to the center of the earth with its projection on the plane. Positive for northern hemisphere Negative for southern hemisphere

Page 14: 4. Energy Meteorology (EEE 483)

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Declination angle, δ: The angular displacement of the sun from the plane of the Earth’s equator. Positive when measured above the equatorial plane in thenorthern hemisphere. The declination angle can be approximately determine from the

equation.

Solar Radiation Geometry

Page 15: 4. Energy Meteorology (EEE 483)

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Hour Angle, ω: The hour angle is the quantity which describe the solar time in trigonometric relationship. It is equal to the angular displacement of the sun from local meridian due to the rotation of earth. Earth completes one rotation in 24 hours. Therefore one hour

corresponds to 15o of rotation. At solar noon, hour angle is zero. It is –ve in the forenoon and +ve in the

afternoon.

ω = [solar time-12.00] in hour x 15 degree

Solar Radiation Geometry

Page 16: 4. Energy Meteorology (EEE 483)

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Inclination Angle, : The angle between the sun’s ray and its projection on a horizontal surface is known as the inclination angle

Zenith Angle, θz: It’s the angle between the sun’s ray and the perpendicular (normal) to the horizontal plane.

Solar Radiation Geometry

Page 17: 4. Energy Meteorology (EEE 483)

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Solar Azimuth Angle( γ): The angle on a horizontal plane, between the line due south and the projection of the sun’s ray on the horizontal plane. It is positive taken from south towards west.

Slope (Tilt angle): It is the angle between the inclined plane surface (collector), under consideration and the horizontal.

Solar Radiation Geometry

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Angle of incidence (θi):

Slope angle varies 0o to 90o.

For Horizontal surface: β=0(cosβ=1, sinβ=0)

For Vertical surface. β=90o, γ=180 for northern hemisphere, 0 for southern hemisphere.

Solar Radiation Geometry