Document ZJjoNm44VxE4DV2MNy4zXxY17

2.60: QHAPTER 12 1956 Guide tieularly' important;, as the temperature gradient from .floor to breathinglevel to ceiling may. depend to . a .large extent,on whether .direct radiation, unit heaters or warm air is used, and in the latter casey whether the air is moved mechanically or by gravity. The temperature of the heating medium is also a factor. ' r It is impracticable to establish rigid rules for determining the temperature difference to use in all cases. However, for residences and structures hav ing ceiling heights under 10 ft,. the comparatively small temperature differential between the breathing level and ceiling generally may be Table 3 Approximate Temperature Differentials Between Breathing Level and Ceiling, Applicable to Certain Ttpes op Heating Systems* Breathing Level Temperatube (5 ft Above Floor) Height CFt): 60 65 70 72 74 ' 76 78 80 85 '90/ v15 : * `7 20 .. 5Q. -. 3.0 3.6 4.2 4.8 5.4 6.0 6.1 6.2 6.3 6.4 6.5 7.0 7.5 8.5 9.5 3.3 3.9 4.6 5.2 5.9 6.5 6.6 6.7 6:8 6.9 7.0 7.58.0 8.5 9.0 9.5 10.0 3.5 3.6 3.7 4.2 4.3 4.4 4.9 5.0 5.2 5.6 ? 5.8 S.9 6.3 6.5 6.7 7.0 7.2 .. 7.4 3.8 4.6 5.3 6.1 6.8 7.6 7.1 7.2 7.3 7.4 7.5' 7.3 7.4 7.5 7.6 . 7.7 ~ 7.5 7.6 7.7 7.8 7.9 7.7 - 7.. 8 7.9 8.0 8.1 8.0 8.2 - 8.4 8.6 8.5 8.7 - 8.9 9.1 9.0 9.2- f ' 9.4 9.6 9.5 9.7 9.9 10.1 10.0 10.2 10.4 . 10.6 10.5 10.7 10.9 . 11.1 3.9 4.0 3.7 `.4.8 5.5 5.6 6.2 ' 6.4 7.0 - 7.2 ' 7.8 8.0 7.9 8.0 . 8.1 8.2 8.3 8.1 8.3 8.5/: "8.4 8.5 8.8 9.3 9.8 10.3 10.8 11.3 9.0 9.5 10.0 10.5 11.0 11.5 4.3 . 5.1 ;6.8 4.5' 5.4. 6.3.7.2. ' 8.5, 9.0 8.6 . 9.1 .. 9;3 9.4 . 9.5 10.5 11.0 U-5 .12.0 10.0 il .5 12.5 * The figures in this table are based onan increase of 2 percent per foot of height above the breathing level (5 ft) up to 15 ft and Mo of one degree for each foot above 15 ft. This table is generally applicable to forced air types of heating systems. For direct radiation or gravitywarm air, increase values 50 percent to 100 percent. neglected without serious error. For higher ceilings, an allowance of approximately 1 percent per foot of height above the breathing level may be made for ceding heights up to 15 ft and approximately x!o of 1 "deg'per foot of height above this level. The values in Table 3 are calculated on this basis. For direct radiation and gravity warm air systems, the allow ance should be increased from 50 percent to 100 percent over those given in Table 3. These, rules should, however, be used with considerable dis cretion, and they do not apply, to some types: of heating systems such as those using panel and baseboard'.;radiation, where very low. temperature differences between: the, floor and the ceiling may exist. Temperature at Floor Level. According to tests at the University of Illinois,3' * 6' 6 the temperature at the floor level ranged from about 2 to 6 deg below that at the breathing level, or somewhat greater than the difference between the breathing level and ceiling temperatures. Tests at the University of Wisconsin1 indicated; a somewhat smaller ^differential between the floor and breathing level temperatures. As a general rule, if the breathing level to ceiling temperature differential-is neglected (as with ceiling heights under 10 ft), the breathing level to floor differential may also be neglected, as the two are somewhat compensating, especially where both floor and ceiling losses are calculated for the same space. In other cases, the 10 ft temperature differentials in Table 3 may be used in arriving at the floor heat loss, these differentials to be subtracted from the breathing level temperature. Heatmg Load 261 ATTIC TEMPERATURES Frequently, it is necessary to estimate the attic, temperature, and in such cases Equation 1 can be used for this purpose: u ^ AM.ti 4-' t0(A,U, -f .A.H. + AJ7.) (D where / = attic temperature, Fahrenheit degrees. - \ ii = inside temperature near top floor ceiling, Fahrenheit degrees. tQ -- outside temperature, Fahrenheit degrees. . : Ac = area of ceiling, square feet. A, = area of roof, square feet. , . ,, /. = area, of net vertical attic1 wall surface, square feet. AR = area of attic glass, square feet. , ;. Uc = coefficient of transmission of ceiling, based on-surface-conductance of 2.20 (upper surface> see Chapter 9). 2.20 = reciprocal of one-half the air space resistance.. ~ U, = coefficient of transmission of roof, based on surface conductance of 2.20 (lower surface, see Chapter 9). . .............. U* = coefficient of transmission of vertical wall surface. Vt = coefficient of transmission of glass. Exam-pie 1. Calculate the temperature in an unheated attic, assuming the follow ing conditions: i, = 70; Jo =10; Ac = 1000; A, = 1200; A,.= 100; A,, = 10; TJ, = 0.50; Ug = 0.40; U, = 0.30; XJg = 1.13. Solution: Substituting these values in Equation 1: . (1000 X 0.40 X 70) -f 10[(1200 X 0-50) 4- (100 X 0.30) + (10 X 1.13)] (1000 X 0.40) + (1200 X 0.50) + (100 X 0.30) + (10 X 1.13) 34,413 J = = 33.1 F. 1041 Equation 1 neglects the effect of any interchange of air such as would take place through attic vents or louvers intended to preclude attic con densation. However, according to tests,8 such venting of attics by means of small louvers or other small openings does not appreciably reduce the attic temperature and may be neglected without serious-error. Neither does this equation take into consideration such factors as heat exchange between chimney and attic or solar radiation to and from the roof. Because of these latter effects, actual attic temperatures are fre quently higher than the calculated values using Equation 1. The attic temperature may be calculated in the usual manner by means of Equation 1_> allowing the full value of the roof. The error resulting from this assump tion will generally be considerably less than if the roof were neglected (as is sometimes the practice) and the attic temperature assumed to be the same as the outside temperature. When relatively large louvers are installed, ss is customary in the southern states; the attic temperature is often as- temed as the: average between inside and -outside. Per a shorter, approximate method of calculating heat losses through