
Heating
 Load
 Calculations
Structure
 heat load
 is
 composed
 of (1)
 transmission
loss through walls, windows,
 and
 roof
 and (2)
 infiltra-
tion
 of
 cold outside air, which must
 be
 heated
 to the
design space temperature.
The
 transmission loss through
 any
 portion
 of the
structure
 envelope
 is
H
 = U x A x
 A7
 (23-4)
where,
 in SI
 units,
 H is the
 heat loss
 in
 watts
 per
 hour,
U
 is the
 overall heat transmission coefficient
 in W/
(m
2
 • h •
 0
C),
 A is the
 surface area
 in
 square meters,
 and
AT
 is the
 inside-to-outside temperature difference
 in
degrees Celsius.
 In
 U.S. customary units,
 H is in
 Brit-
ish
 thermal units
 per
 hour,
 U is in
 Btu/(ft
2
 • h •
 0
F),
 A is
in
 square
 feet,
 and
 A7
 is in
 degrees Fahrenheit. Trans-
mission
 coefficients
 for
 typical walls, windows,
 and
roofs
 as
 well
 as
 methods
 of
 calculating
 the
 coefficient
for
 the
 combinations
 of
 materials
 are
 given
 in
 Chapter
25 of the
 ASHRAE Handbook
 of
 Fundamentals
 [12].
Cooling
 Calculations
Heat gain throughout
 the
 structure, which makes
 up the
external cooling load,
 is
 more
 difficult
 to
 calculate than
heat
 loss because
 of the
 effects
 of
 radiated heat
 from
 the
sun.
 This additional heat source must
 be
 considered
 in
addition
 to the
 heat gain
 by
 conduction
 due to the
 differ-
ence between outdoor
 and
 indoor temperatures. Sunlight
does
 not
 heat space
 air
 directly,
 but it
 raises
 the
 tempera-
ture
 of
 sunlit
 surfaces
 as a
 result
 of
 absorbed radiation.
Many
 factors
 influence
 the
 amount
 and
 timing
 of
solar heat reaching
 the
 space.
 The
 intensity
 of
 incident
solar radiation depends
 on
 latitude, time
 of
 year, time
of
 day, cloud cover,
 and
 atmospheric pollution.
 The
time
 lag
 between solar heat input
 and
 interior
 air
 tem-
perature rise
 may
 vary
 from
 a few
 minutes
 to
 several
hours.
 The lag is
 affected
 by the
 surface color
 of the
exterior,
 the
 heat storage capacity
 and the
 insulating
value
 of the
 construction,
 and the
 daily outdoor tem-
perature
 range, among other
 factors.
The
 combined heat
 from
 both
 the
 higher outdoor
temperature
 and
 solar radiation moves progressively
through
 walls
 and
 roof,
 finally
 raising
 the
 interior sur-
face
 temperatures. Loss
 from
 those surfaces occurs
 by
radiation
 to
 cooler
 surfaces
 and by
 convection
 to the
adjacent
 air.
 Air
 warmed
 by
 convection expands,
becomes lighter, rises,
 and is
 replaced
 by
 cooler
 air,
which
 continues
 the
 convective process.
Except
 for
 minor reflected losses, sunlight passes
directly
 through clear glass
 and is
 absorbed
 by the
interior
 surfaces
 it
 strikes. Their increased tempera-
ture
 transfers heat
 to
 other
 cooler
 surfaces
 by
 reradia-
tion
 and to the air by
 convection.
Simply stated, solar heat gain
 is
 taken into account
 by
using
 a
 higher outdoor temperature than actually would
exist
 at the
 time considered
 for
 each heat gain calcula-
tion.
 The
 ASHRAE
 Handbook
 of
 Fundamentals
 [12]
contains tables
 of
 cooling load temperature
 differential
(CLTD)
 data (for
 use in
 calculating conduction heat gain
through
 sunlit walls
 and
 roofs)
 and
 cooling load
 factors
(CLF) (for calculating
 the
 solar radiation through glass).
Both
 sets
 of
 data include
 the
 effect
 of
 time delay
 due to
thermal storage.
 The
 total resistance
 to
 heat
 transfer
 for
each type
 of
 construction
 is
 found
 by
 adding
 the
 resis-
tances
 of its
 components,
 as
 illustrated
 in
 Example
 23-1.
Peak
 Heat
 Gain
The
 peak heat gain
 to a
 space
 is the
 largest
 sum of
external
 and
 internal
 heat gains that occur simulta-
neously.
 Heat removal capacity,
 in the
 form
 of
 ventila-
tion
 or
 cooling, equal
 to the
 peak heat gain must
 be
available
 to
 maintain
 the
 design space temperature.
External heat gain results
 from
 an
 outdoor tempera-
ture that
 is
 higher than
 the
 indoor temperature
 as
 well
as
 from
 solar radiation. Internal heat gain comes pri-
marily
 from
 operating motors
 and
 engines.
Air
 Intake
 and
 Exhaust
 Openings
Intakes
 for
 ventilation
 air
 should
 be
 through
 screened
louvers that exclude rain, snow, birds,
 and
 insects.
Ducted intakes that
 are
 connected
 to
 air-handling units
with
 filters
 that exclude insects need only bird screens.
Nonducted intakes should include insect screens
 or
filters.
 All
 screens
 and filters
 must
 be
 readily
 accessi-
ble for
 cleaning
 or
 replacement. Bird screens
 do not
need mesh openings smaller than
 25 mm
 (
1
I
2
 in.).
 The
air
 resistance
 of filters
 used
 at
 unducted wall intakes
should
 not
 exceed
 24 Pa
 (0.1
 in. WC)
 when clean
 to
limit negative pressure
 in the
 space
 (created
 by
exhaust
 fans)
 to 63 Pa
 (0.25
 in.
 WC);
 low
 negative
pressure makes doors easier
 to
 open
 and
 close.
 Both
the
 louver
 and
 screen should
 be
 constructed
 of a
 cor-
rosion-resistant material
 or
 should have
 a
 corrosion-
protective coating. Provide
 an
 intake damper
 at
 each
louver
 in
 cold climates, preferably with positive clo-
sure
 on
 failure
 of its
 pneumatic
 or
 electric actuator.
Hurricane-prone locations
 may
 warrant
 an
 additional
manually
 operated damper
 (on the
 outdoor
 air
 intake)
that
 can be
 locked closed when
 a
 storm approaches.
Air
 exhaust openings should
 be
 protected
 from
 the
weather
 by a
 wall louver, hood, penthouse,
 or
 weather