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OD DVOSTRUKO ZASTAKLJENOG PROZORA DO DVOSTRUKE FASADE – INDIKATORI PRENOSA
TOPLOTE STACIONARNOG STANJA
FROM DOUBLE-GLAZED WINDOW TO DOUBLE-SKIN FACADE – STEADY STATE HEAT TRANSFER
INDICATORS
Gabriel NĂSTASEAlexandru ȘERBANGeorge DRAGOMIR
Sorin BOLOCANAlin Ionuț BREZEANU
46. Međunarodni kongres i izložba o KGH, Beograd, 2–4. Decembar 201546th International HVAC&R Congress and Exhibition, Belgrade, 2–4 December 2015
CIVIL ENGINEERING FACULTY, BUILDING SERVICES DEPT., BRAȘOV, ROMANIA
46. Međunarodni kongres i izložba o KGH, Beograd, 2–4. Decembar 201546th International HVAC&R Congress and Exhibition, Belgrade, 2–4 December 2015
The envelope (façade) is the part of the building which forms the primary
thermal barrier with its environment. It represents the most important factor in
determining the level of comfort, natural lighting and ventilation ability, and
finally how much energy is needed for heating and air –conditioning [1]. The
main purpose of this study is to identify and emphasize the difference between
single-skin façade and double-skin façade from heat transfer point of view. For
this purpose were taken into account total thermal resistances, transmittances
and heat fluxes.
I. INTRODUCTION
46. Međunarodni kongres i izložba o KGH, Beograd, 2–4. Decembar 201546th International HVAC&R Congress and Exhibition, Belgrade, 2–4 December 2015
Designing a double glazed façade entails the detailed analysis of
several variables and then their implementation in a model which can be
subjected to a simulation which can take into account the atmospheric condition
for a one-year period in order to make decisions related to the optimal
configuration of a double glazed façade and also to the operation method and
the strategies for controlling it.
In double glazed façades the heat transfer involves several phenomena
which occur simultaneously and which overlap. A schematic model of the heat
transfer through a double glazed façade (b) and (c) is shown in Figure 1, in
comparison with heat transfer through a double pane window (a).
46. Međunarodni kongres i izložba o KGH, Beograd, 2–4. Decembar 201546th International HVAC&R Congress and Exhibition, Belgrade, 2–4 December 2015
Heat transfer illustrated in Figure 1 include direct and diffuse solar
radiation, conduction, convection, and long-wave radiation.
(a) (b) (c)
Heat transfer in double pane window and in double skin façade, without and with shading device inside cavity.
46. Međunarodni kongres i izložba o KGH, Beograd, 2–4. Decembar 201546th International HVAC&R Congress and Exhibition, Belgrade, 2–4 December 2015
II. DOUBLE-GLAZED WINDOW HEAT TRANSFER
ALGORITHM
• double glazing with the height of 2 m;
• the heat transfer considered during the
night;
• the effect of the solar radiation can be
ignored;
• in stationary regime and in one direction;
• and the effect of the casement is ignored.
46. Međunarodni kongres i izložba o KGH, Beograd, 2–4. Decembar 201546th International HVAC&R Congress and Exhibition, Belgrade, 2–4 December 2015
The expression of the global unitary flow for the proposed case has the
expression [3]:
recegegerbcbgigirici
oi
hhkhhkhh
TT
A
Q
11111
(1)
46. Međunarodni kongres i izložba o KGH, Beograd, 2–4. Decembar 201546th International HVAC&R Congress and Exhibition, Belgrade, 2–4 December 2015
The global unitary flow is usually expressed by the global heat transfer
coefficient U:
(2))( oioi TTU
R
TT
A
Q
46. Međunarodni kongres i izložba o KGH, Beograd, 2–4. Decembar 201546th International HVAC&R Congress and Exhibition, Belgrade, 2–4 December 2015
Comparing equations (1) and (2) it follows R=1/U that is [3]:
(3)
recegegerbcbgigirici hhkhhkhhR
11111
46. Međunarodni kongres i izložba o KGH, Beograd, 2–4. Decembar 201546th International HVAC&R Congress and Exhibition, Belgrade, 2–4 December 2015
The value of the convective thermal transfer coefficient in the space
between the two glass sheets is then obtained with the formula:
b
cbk
LNuh
(4)
where kb is the thermal conductivity of the gas between the two glass sheets [3].
The thermal conductivity kb is evaluated at the average temperature from the
space between the two sheets namely Tbm=T2+T3.
46. Međunarodni kongres i izložba o KGH, Beograd, 2–4. Decembar 201546th International HVAC&R Congress and Exhibition, Belgrade, 2–4 December 2015
III. FROM DOUBLE-GLAZED WINDOW TO DOUBLE-
SKIN FAÇADE
The exterior envelope is represented in the case of most double-skin facades by secure
glass; its thickness may vary between 8 and 12 mm. The main role of the exterior envelope is
to offer the entire construction adequate resistance against exterior climatic conditions, at the
same time contributing to good acoustic insulation for the entire building.
The cavity of the double façade which is located between the exterior cover and the
interior one is an intermediary air layer whose thickness can range between 25 cm and 2 m.
The role of this intermediary air layer is to contribute to the increase of the thermal insulation
degree of the entire façade, at the same time offering the possibility that, in certain conditions,
air can be preheated inside it for the building’s natural or mechanical ventilation.
46. Međunarodni kongres i izložba o KGH, Beograd, 2–4. Decembar 201546th International HVAC&R Congress and Exhibition, Belgrade, 2–4 December 2015
Heat transfer in double-skin
façade and temperature
distribution during cold
season
46. Međunarodni kongres i izložba o KGH, Beograd, 2–4. Decembar 201546th International HVAC&R Congress and Exhibition, Belgrade, 2–4 December 2015
Further on we suggest the extension of the method used for double
glazed window with the final purpose of determining the total heat
flow, which horizontally passes through the entire double glazed façade
system, consisting of the three components, the exterior envelope, the cavity
and the interior envelope.
The calculation is also made in an iterative way by determining a
convective coefficient and a radiation one for the cavity and afterwards we
obtain the conductive resistance through the secure glass as well as the
convective and radiation resistance at the exterior surface of the secure glass,
which is in contact with the exterior air.
46. Međunarodni kongres i izložba o KGH, Beograd, 2–4. Decembar 201546th International HVAC&R Congress and Exhibition, Belgrade, 2–4 December 2015
In case of double-skin façade equation (2) remains the same but
in equation (3) and respectively in (1) we have two more terms and
equation (3) can be written as:
recegsgsrcavccavgegerbcbgigirici hhkhhkhhkhhR
1111111
(5)
46. Međunarodni kongres i izložba o KGH, Beograd, 2–4. Decembar 201546th International HVAC&R Congress and Exhibition, Belgrade, 2–4 December 2015
IV. CONCLUSIONS
As can be seen the difficult part of this calculation is to determine convection
superficial heat transfer coefficients, for both inner envelope and for the double-skin cavity.
This coefficient varies depending on the type of envelope chosen for the interior of the
double façade and for the cavity it depends on ventilation mode, which can be natural,
mechanical or hybrid. As indicated in literature the energy performance of a double-skin
façade depends on various aspects as location, orientation, climatic conditions, type of inner
and outer envelope, thermophysical properties of materials included, type of double-skin
façade, type of ventilation inside cavity, control strategies. Study of steady state heat transfer
can provide first information on the impact of adopting a double glass facade to a certain
building but for this purpose it is important to create an universally classification for such
system.
THANK YOU VERY MUCH!!
Gabriel NĂSTASEAlexandru ȘERBANGeorge DRAGOMIR
Sorin BOLOCANAlin Ionuț BREZEANU
46. Međunarodni kongres i izložba o KGH, Beograd, 2–4. Decembar 201546th International HVAC&R Congress and Exhibition, Belgrade, 2–4 December 2015
CIVIL ENGINEERING FACULTY, BUILDING SERVICES DEPT., BRAȘOV, ROMANIA