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268
CHAPTER 12
1951 Guide
] representative of a clear summer day at sea-level elevation, and are nearly identical with values derived from suggested design sol-air temperatures for Lincoln, Nebraska.3 Values typical of a humid industrial area derived
1 from sol-air data for New York City4 are also given in Table 5. Day-to, day changes in the amount of dust and water vapor in the atmosphere I cause large differences in solar intensity values observed on cloudless days 1 at a given locality. For example, it has been observed in Cleveland that '! values of the order of those given for industrial atmospheres are usually associated with dry-bulb and wet-bulb temperatures near the design | values of 95 F and 75 F (67 F dew-point). On the other hand, values | approaching or exceeding those for a clear atmosphere are often encountered I during Cleveland summers, but with dew-point and maximum dry-bulb i temperatures 10 to 15 deg lower. Considerable judgment, therefore, is j, required in selecting solar intensity values for design purposes.
Data regarding the irradiation of vertical and horizontal surfaces by f diffuse or sky radiation are few. Suggested design values for a 40-deg
latitude on August 1 (18 deg declination, north) are given in Table 5 for |! the two types of atmospheres. These are based upon observations made j on cloudless days in Cleveland over a period of several summers. Since j less extensive data were available for industrial atmospheres, there is more 1 j uncertainty regarding these values. In both instances,' the values include j! . an unknown amount of ground reflection, which may be expected to vary
with location. It should be noted that clouds which do not obscure the li sun tend to increase diffuse radiation values. Nearby buildings may reduce , diffuse irradiation by partial shading.
Calculation Tables
The irradiation of a surface by the sun is the product of 7dq, the direct normal radiation (see Table 5), and the cosine K of the incident angle, 8. |: For horizontal surfaces, the cosine K equals the sine of the solar altitude, i. For vertical walls, if is a function of the solar altitude /S and the wall ]t solar azimuth y, thus
!'
K = cos 8 = cosp cos y
(1)
!i These three angles are defined in Fig- 1. Values of K are given in Table 6 !j and values of d and y are given in Table 7 for 18 deg north declination j; (August 1).
To compute K values for orientations other than those given in Table 6, |ji third angle <f>, the solar azimuth, is required. In this discussion, will be I measured east from south in the morning, and west from south in the after-
:l noon. Hence, <j> values are equal to 90 deg minus the y values for an east ; or west facing wall, except when Table 7 shows the south walls to be in the
shade. In this case <t> equals 90 + y, that is, <f> is greater than 90 deg.
; The wall azimuth rp is the angle, 'measured east from south to the peri pendicular to the wall for walls which have an easterly component, and west 'i from south for those having a westerly component. For example, ^ for a :! wall facing northeast is 135deg.
j The wa.ll solar azimuth y may be found according to the following
i; schedule:
I
!ii
For walls facing east of south:
For walls facing west of south:
jj
-y = ^ ^ a.m.
y = <f> + ip a.m.
]:
y = <t> +1 p.m.
y = 4> -- p p.m.
Cooling Load
269
' fi'i Values of K, the Cosine of the Incident Angle, fob Vabiously
Table o.
Obibnted Walls and a Hobizontal Surface
Computed for 18 Deg Declination, North (August 1)
Son Time
AMi
6 aJR. 6 P**
t7 f
s
10 2 11 1 ' - 12
pi-
N 0.267 0.144 0.030
N
30 Dso North Latitude Cosine K of the Incident Anode
NE E SE 8
0.862 0.752 0.604 0.427
0.234 0.039
0.952 0.919 0.824 0.672
0.476 0.246 0.000
0.484 0.548 0.561 0.524
0.438 0.310 0.147
0.068
0.144 0.192 0.208
NW W sw
S
SW
0.147 SE
Hobiz.
0.156 0.367 0.566 0.737
0.866 0.951 0.978
Hobiz.
Sun Time
am1 5 a.m. 7 pjn.
8*
10 2 12 -- t
PM --
N 0.406 0.237 0.079 .
N
Sun Time AM-
i
84
N 0.385 0.199 0.010
12 t
PM --
.N
40 Deo North Latitude Cosine K or the Incident Angle
NE E SE 8
0.934 0.840 0.705 0.533
0.337 0.129
0.914 0.951 0.919 0.824
0.673 0.475 0.246 0.000
0.358 ` 0.505
0.594 0.631
0.614 0.542 0.424 0.265
0,069
0.198 0.292 0.354 0.375
NW W SW S
SW
Hobiz.
0.076 0.265
0.009 0.199 0.391 0.566
0.713 0.829 0.903 0.927
SE ` Hobiz.
60 Deo North Latitude Cosine K or the Incident Angle
NE E SE s
0.922 0.813 0.656 0.465
0.252 0.030
0.920 0.951 0.918 0.824
0.673 0.475 0.247 0.000
0.378 0.532 0.643 0.700
. 0.699 0.642 0.532 0.375
0.166
0.316 0.433 0.505 0.530
NW W
SW
S
SW
0.183 0.375 SE
Hobiz.
0.078 0.233 0.399 0.545
0.669 0.766 0.829 0.848
Hobiz.
Treat negative values of y as if they were positive. If 7 is greater than 90 deg, the wall is in the shade.
Values of K for other seasons and latitudes may be found in the litera ture,5 or may be computed from data given in Hydrographic Office Bulletin No. 214, Tables of Computed Altitude and Azimuth6 and the Ephemeris of the Sun.7 Table 8 shows the variation of solar declination during the months ordinarily requiring cooling.
Example 1: Find the solar azimuth at 6:30 p.m. at 40 deg north latitude on August 1st.
Solution. From Table 7 in the column of y for a wall facing west <f> for 6DO p.m.