Hygiene: a manual of personal and public health (New Edition)Newsholme, Arthur, Sir
Science
Hygiene: a manual of personal and public health (New Edition)
Newsholme, Arthur, Sir
Hygiene; Public health -- Great Britain; Sanitation
It is desirable to make each individual inlet not larger than 48 to
60 square inches in area, _i.e._ large enough for two or three men;
and each outlet not larger than one square foot, or enough for six men
(Parkes). This ensures more uniform diffusion of the air throughout
a room. On the other hand, the loss by friction is greatly increased
by having a number of small openings instead of one large opening.
This loss is inversely to the square roots of the respective areas.
Thus the square root of 100 is 10; the sum of the square roots of the
four apertures of 25 square inches each is 20. The loss by friction is
double in the second case what it was in the undivided opening. It is
evident, therefore, that in order to get as much air through the four
openings as through the original large opening, each must be equal in
size to half the original opening.
_Why is ventilation more difficult in upper rooms of large houses and
in single-storied houses than in the lower storeys of large houses?_
Cold external air being heavier than the internal warm air presses
downwards to the lowest point, and pushes up the warmer air. If there
were a vacuum in the room, air would rush into it with a velocity
which, as seen before, is represented by the formula—
v = √(2_gs_).
Where g = 32, s = height of column of air, which we may take as roughly
5 miles.
From this formula we obtain v = 1,306 feet per second.
It is evident that in such a case the velocity of entry of air into a
vacuum on the ground floor would be greater than into a vacuum on any
of the higher storeys, owing to the greater velocity acquired through
the increased action of gravity.
And the same increased facility of entry of air into lower rooms must
hold good under ordinary circumstances, inasmuch as by Montgolfier’s
formula (which is founded on the fundamental formula v = √(2_gs_)
v = √(2_gh_(t-t^1)/492)
h = distance between top of chimney and floor of room in question, and
thus the velocity with which air enters is governed by the difference
between the internal and external temperature, and the height from
which the cold air descends in order to take the place of the air which
has escaped.
CHAPTER XXII.
METHODS OF VENTILATION.
In most houses no special means of ventilation are provided, windows,
doors and fire-places being trusted for ensuring a sufficient supply
of fresh air. These do not suffice in well-built houses, unless
the inhabitants train themselves into enduring the currents of air
necessarily associated with open windows and doors. They are, however,
aided in the majority of houses by the porosity of walls, by currents
of air through crevices of wood-work, and so on. It is desirable that
adequate special provision for ventilation should be made for every
house when it is built, and that as much care and forethought should
be exercised in this respect as in the laying on of a water-supply or
sanitary appliances connected with drainage.
Public-domain text, read in full here on John Shaqi.
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