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Handbook of air conditioning and refrigeration / Shan K

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3.24 CHAPTER THREE<br />

● Solar altitude angle � (Fig. 3.7a <strong>and</strong> b) is the angle ROQ on a vertical plane between the sun’s ray<br />

OR <strong>and</strong> its projection on a horizontal plane on the surface <strong>of</strong> the earth.<br />

● Solar azimuth � (Fig. 3.7a) is the angle SOQ on a horizontal plane between the due-south direction<br />

line OS <strong>and</strong> the horizontal projection <strong>of</strong> the sun’s ray OQ.<br />

● Solar declination angle � (Fig. 3.6) is the angle between the earth-sun line <strong>and</strong> the equatorial<br />

plane. Solar declination � changes with the times <strong>of</strong> the year. It is shown in Fig. 3.6 on June 21.<br />

● Surface-solar azimuth � (Fig. 3.7a <strong>and</strong> c) is the angle POQ on a horizontal plane between the<br />

normal to a vertical surface OP <strong>and</strong> the horizontal projection <strong>of</strong> the sun’s rays OQ.<br />

● Surface azimuth � (Fig. 3.7a) is the angle POS on a horizontal plane between OP <strong>and</strong> the direction<br />

line SN.<br />

● Latitude angle L (Fig. 3.6) is the angle S�O�O on the longitudinal plane between the equatorial<br />

plane <strong>and</strong> the line O�O that connects the point <strong>of</strong> incidence <strong>of</strong> the sun’s ray on the surface <strong>of</strong> earth<br />

O <strong>and</strong> the center <strong>of</strong> the earth O�.<br />

Hour Angle <strong>and</strong> Apparent Solar Time<br />

Solar Angle Relationships<br />

Hour angle H (Fig. 3.6) is the angle SOQ on a horizontal plane between the line OS indicating the<br />

noon <strong>of</strong> local solar time t ls <strong>and</strong> the horizontal projection <strong>of</strong> the sun’s ray OQ. The values <strong>of</strong> the hour<br />

angle H before noon are taken to be positive. At 12 noon, H is equal to 0. After 12 noon, H is negative.<br />

Hour angle H, in degrees, can be calculated as<br />

H � 0.25 (time in minutes from local solar noon) (3.49)<br />

The relationship between apparent solar time t as, as determined by a sundial <strong>and</strong> expressed in apparent<br />

solar time, <strong>and</strong> local st<strong>and</strong>ard time t st, both in minutes, is as follows:<br />

(3.50)<br />

where M � local st<strong>and</strong>ard time meridian <strong>and</strong> G � local longitude, both in degrees. In Eq. (3.50), t eq,<br />

in minutes, indicates the difference in time between the mean time indicated by a clock running at a<br />

uniform rate <strong>and</strong> the solar time due to the variation <strong>of</strong> the earth’s orbital velocity throughout the year.<br />

The relationship among the solar angles is given as<br />

sin� � sin� sinL � cos� cosH cosL (3.51)<br />

<strong>and</strong><br />

Angle <strong>of</strong> Incidence <strong>and</strong> Solar Intensity<br />

t as � t eq � t st � 4(M � G)<br />

cos � �<br />

sin� sin L � sin �<br />

cos� cos L<br />

(3.52)<br />

The angle <strong>of</strong> incidence � (Fig. 3.7a) is the angle between the sun’s rays radiating on a surface <strong>and</strong><br />

the line normal to this surface. For a horizontal surface, the angle <strong>of</strong> incidence � H is ROV; for a vertical<br />

surface, the angle <strong>of</strong> incidence � V is ROP; <strong>and</strong> for a tilted surface, the angle <strong>of</strong> incidence � � is<br />

ROU. Here, � is the angle between the tilted surface ABCD <strong>and</strong> the horizontal surface.<br />

Let I DN be the intensity <strong>of</strong> direct normal radiation, or solar intensity, on a surface normal to the<br />

sun’s ray, in Btu/h�ft 2 (W/m 2 ). In Fig. 3.7b, I DN is resolved into the vertical component RQ � I DN

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