Heiselberg, Per

Nielsen, Peter V.

Svidt, Kjeld

English

This paper describes the results of laboratory measurements of the airflow from a bottom hung window mounted near the ceiling of a ventilated room. In the laboratory set-up it was possible to control the temperature difference and the airflow rate through the window. The pressure drop through the window was measured as well as the velocity distribution in the incoming airflow. Airflow patterns and penetration depth of a cold jet were studied with smoke visualisation

    Aalborg UniversitetCharacterization of the Airflow from a Bottom Hung Window under Natural VentilationSvidt, Kjeld; Heiselberg, Per; Nielsen, Peter V.Publication date:2000Document VersionPublisher's PDF, also known as Version of recordLink to publication from Aalborg UniversityCitation for published version (APA):Svidt, K., Heiselberg, P., & Nielsen, P. V. (2000). Characterization of the Airflow from a Bottom Hung Windowunder Natural Ventilation. Dept. of Building Technology and Structural Engineering, Aalborg University. IndoorEnvironmental Engineering Vol. R0041 No. 116General rightsCopyright and moral rights for the publications made accessible in the public portal are retained by the authors and/or other copyright ownersand it is a condition of accessing publications that users recognise and abide by the legal requirements associated with these rights.            ? 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Q) -c: J:: -1'-0 0 0 N 1-z w > ~ 0 0 0:: .... 0 (/) Ol .f: "0 Q) Q) t) e 0.. .£ '::i ::::> c; .f: "0 ro Q) 0:: fli E 0 0 0 0:: CD 1'-.f: I lt) c: lt) 0 1'-:;::::; :::J ci. .0 c. ·c: ii5 -i5 g .... ~ 0 c: 0 0 0 Q) N t) N" c: Q) ...... .... I ~ cr> c: >. 0 "3 () """") The Indoor Environmental Engineering papers are issued for early dissemination of research results from the Indoor Environmental Engineering Group at the Department of Building Technology and Structural Engineering, Aalborg University. These papers are generally submitted to scientific meetings, conferences or journals and should therefore not be widely distributed. Whenever possible, reference should be given to the final publications (proceedings, journals, etc.) and not to the Indoor Environmental Engineering papers. Printed at Aalborg University Characterization of the ... ~ Airflow from a Bottom Hung Window under Natural Ventilation K. Svidt, P Heiselberg, P V. Nielsen ABSTRACT CHARACTERIZATION OF THE AIRFLOW FROM A BOTTOM HUNG WINDOW UNDER NATURAL VENTILATION Kjeld Svidt, Per Heiselberg and Peter V. Nielsen Department of Building Technology and Structural Engineering, Aalborg University, Sohngaardsholmsvej 57, 9000 Aalborg, Denmark For natural ventilation of rooms there is a wide range of possibilities with regard to the selection of window type, size and location. A bottom hung window mounted near the ceiling is often used as it has proved to work well with regard to draught risk and thermal comfort in the room. However, there is a need for more detailed information on the performance of this and other types of windows to make it possible to use improved design methods for natural ventilation systems. This paper describes the results of laboratory measurements of the airflow from a bottom hung window mounted near the ceiling of a ventilated room. In the laboratory set-up it was possible to control the temperature difference and the airflow rate through the window. The pressure drop through the window was measured as well as the velocity distribution in the incoming airflow. Airflow patterns and penetration depth of a cold jet were studied with smoke visualisation. KEYWORDS Natural ventilation, windows, air velocity, air distribution, cold jet, penetration depth, full -scale laboratory measurements. INTRODUCTION In buildings ventilated by natural or hybrid ventilation the air is often supplied and in some cases exhausted through open windows. There is a need for information on the performance of such windows to make it possible to use improved design methods for natural ventilation systems. This study focuses on the airflow from a bottom hung window which acts as an inlet only, i.e. no air is exhausted through the window. The window is tested at different opening sizes, inlet velocities and different indoor and outdoor temperatures. Velocity characteristics of the inlet air jet have been studied under isothermal conditions and penetration depth of the jet has been studied under non-isothermal conditions. LABORATORY SET-UP The investigations are performed in a laboratory test room with the size of Length x Width x Height = 8 m x 6 m x 3 m, a plane view of the room is showed in Figure 1. The room is divided into two separate rooms by an insulated wall. The small room can be cooled, while the large room can be kept at normal room temperature with a floor heating system. The bottom hung window is mounted in the insulated wall 10 cm below the ceiling (Figure 2). Another window is also mounted in the wall for other purposes (measurements by Heiselberg et al. 1999, 2000). Three different opening areas have been studied. The opening areas were defined as a slot width of 10 mm, 15 mm and 30 mm (see Figure 3 for details). The pressure difference between the two rooms is measured by pressure taps mounted 20 cm below the ceiling beside the window. In the non-isothermal experiments the small room is continuously ventilated by cold air at a flow rate of 1500 m3/h. The airflow rate through the window is controlled by valves in the supply and exhaust ducts. The actual flow rate is determined from previously measured pressure characteristics of the window and leakage characteristics of the room (Heiselberg et al. 1999, 2000). E :::> cri Gold room Experiment room '"' ' ' ~---·-------------1--  , _ _____g,o m -~ ,__ _ __ __ 5,6 m -~ -----.1 Figure 1: The test room is divided into a cold room simulating outdoor conditions and an experiment room with normal room temperature. The window is mounted in the insulated wall between the rooms. 0 ri 0 ,61 -1'----:-1 ~-I g ~-1 I I _____ !~----i------- -+--- ----2_.0 - - ---- -,1 q_ Figure 2: The bottom hung window is mounted in the insulated wall 10 cm below the ceiling. Another window is also mounted in the wall for other purposes. 2 ~a ~/ Figure 3: Section view with details of the window (left), the slot width is measured at the narrowest passage for the flow (in the middle), photo from outside of the window with 30 mm slot opening (right). "" RESULTS Isothennal measurements Under isothermal conditions the inlet flow from the window will form a three-dimensional wall jet along the ceiling. It is assumed that the maximum velocity in the jet follows Eqn. (1): where u u is the maximum velocity at the distance x from the inlet [ m/s] U0 = (2.t1p/ pf-5 is the calculated inlet velocity [ m/s] a0 = qluo is the effective opening area of the window [ m2] Ka is a constant related to the opening X0 is a virtual origin of the jet [m] .t1p is the pressure difference between the rooms [Pa] pis the density of the incoming air [kg!m3] q is the airflow rate through the window [m3/h] The wall jet thickness is assumed to follow Eqn. (2): (1) (2) where £\, is the wall jet thickness at the distance x from the inlet. It is defined as the distance from the ceiling to the height where the velocity is 50% of u. With respect to wall jet thickness the virtual origin is Xoy and Day is the growth rate. 3 Velocity profiles of the wall jet have been measured at eight different distances from the inlet. By rearranging equation 1 the characteristic constants of the jet can be determined graphically as shown in Figure 4. The measurements were performed for two different slot openings h and two different inlet velocities. Table 1 shows the results. There is some variation in the values of Ka and X 0 • If X 0 is fixed to be -2.0 m there is less variation in the calculated values of Ka as shown in the table. TABLE 1 RESULTS OF THE ISOTHERMAL MEASUREMENTS Exp.no h [mm] Lip fPal ao [mk] Ka Xo [m] Ka @x0 = -2.0 Day Xoy 1 15 12 .0236 6.1 -1.6 6.6 .077 -.75 2 15 6 .0222 7.9 -2.5 7.1 .077 -.92 3 30 6 .0396 7.5 -1.9 7.6 .083 -.42 4 30 2.2 .0368 8.1 -2.3 7.6 .073 -.90 3 l ...... - ----- -----5-I I 4.5 2.9 E i ~ -<>-X= 1.0 m 3.5 2.8 I 0 -X-X= 1.5m 3 ;: E -<>-x=2.0m :::1 2.7 "o 0 :::1 .:: ---<>--X=2.5m .. --l>-X = 3.0 m 2 " c 2.6 !!! -1-X=3.5m m -x=4.0m i5 2.5 -x-X=4.5m 2.4 -l----r--.--.----r----.--.----r--.----i 0 0.2 0.4 0.6 0.8 1.2 1.4 1.6 1.8 -3 -2 -1 0 2 3 4 5 Velocity, m/s Distance from inlet Figure 4: Isothermal experiment no 3. Velocity profiles in the centreline of the room (left). Ka and X0 are determined from the regression line (right). Non-isothermal measurements Under non-isothermal conditions the penetration depth of the cold jet has been studied. 55 experiments have been performed at three different slot openings and a number of different inlet velocities as well as two different temperature differences. During each experiment the pressure difference between the rooms is recorded as well as the air temperature in a number of positions in each room. The penetration depth is determined by adding smoke to the air outside the window (Figure 5). Each smoke experiment has been videotaped for documentation. As described by Nielsen et al. (1987) the penetration depth is expected to follow Eqn. (3): K (3) where Xs is the penetration depth and AT a is the temperature difference between inside and outside. 4 Figure 5: The jet penetrates to the distance Xs (left). Photo from smoke experiment no 32 shows where the jet no longer attaches to the ceiling (right). The measured results are plotted in figure 6. It shows that the data fit well with Eqn. (3) within each slot opening. However, it is clear that the curves for each opening differ from each other although the opening area is included in the equation. A possible explanation is that not only the opening area changes when the window is opened more or less, but also the direction of the incoming air is changed. 4.5 ································ ·· ······ ················· ········ ················································ ····································· ······ ··············································································· 4 3.5 3· 2.5 2 1.5 0.5 4 10mm o 15 mm Cl 30 mm --Linear (1 0 mm) --Linear (15 mm) --Linear (30 mm) 0 +---------.---------.----------.---------.---------r---------,--------~ 0 5 10 15 20 25 30 35 Figure 6: Penetration depth results for slot openings 10 mm, 15 mm and 30 mm. 5 CONCLUSION The airflow from a bottom hung window has been analysed under isothermal and non-isothermal conditions. It was found that the incoming air jet under isothermal conditions could be described well with traditional jet theory. The penetration depth of a cold jet from the window matched well with an equation based on the archimedes number of the jet. ACKNOWLEDGEMENT This work is a part of the co-operative work within IEA-ECB&CS Annex 35, Hybrid Ventilation in New and Retrofitted Office Buildings. It has been supported by the Danish Energy Agency. REFERENCES Heiselberg P., Dam H., S0rensen L. C., Nielsen P. V. and Svidt K. (1999). Characteristics of Air Flow through Windows. Presented at the First International One Day Forum on Natural and Hybrid Ventilation, HybVent Forum'99, 09/1999, Sydney, Australia. Heiselberg P., Svidt K., Nielsen PV (2000). Windows, Measurements of Air Flow Capacity. Proceedings of ROOMVENT 2000, July 2000, Reading, UK. Nielsen P.V., Moller A.T.A. (1987). Measurements on Buoyant Wall Jet Flows in Air-Conditioned rooms. Proc. of the First International Conference on Air Distribution in Rooms. ROOMVENT '87. 6 RECENT PAPERS ON INDOOR ENVIRONMENTAL ENGINEERING PAPER NO. 109: E. Bj0rn: Simulation of Human Respiration with Breathing Thermal Manikin. ISSN 1395-7953 R9944. PAPER NO. 110: P. Heiselberg: Hybrid Ventilation and the Consequences on the Development of the Facade. ISSN 1395-7953 R0033. PAPER NO. 111: P. Heiselberg, M. Pedersen, T. Plath : Local Exhaust Optimization and Worker Exposure. ISSN 1395-7953 R0034. PAPER NO. 112: K. Svidt, P. Heiselberg: Push-Pull Ventilation in a Painting Shop for Large SteeiConstructions. ISSN 1395-7953 R0035. PAPER NO. 113: P. Heiselberg: Design Principles for Natural and Hybrid Ventilation. ISSN 1395-7953 R0036 PAPER NO. 114: A. Anderserr, M. Bjerre, Z.D. Chen, P. Heiselberg, Y. Li : Experimental Study of Wind-Opposed Buoyancy-Driven Natural Ventilation. ISSN 1395-7953 R0037 PAPER NO. 115: P. Heiselberg, K. Svidt, P.V. Nielsen: Windows - Measurements of Air FlowCapacity.ISSN 1395-7953 R0040 PAPER NO. 116: K. Svidt. P. Heiselberg, P.V. Nielsen: Characterization of the Airflow from a Bottom Hung Window under Natural Ventilation . ISSN 1395-7953 R0041 PAPER NO. 117: Z. Yue, P.V. Nielsen: Flow Pattern in Ventilated Rooms with Large Depth and Width.ISSN 1395-7953 R0042 . PAPER NO. 118: P.V. Nielsen, H. Dam, L.C. S0rensen, K. Svidt, P. Heiselberg : Characteristics of Buoyant Flow from Open windows in Naturally Ventilated Rooms. ISSN 1395-7953 R0043 . PAPER NO. 119: P.V. Nielsen, C. Filholm, C. Topp, L. Davidson: Model Experiments with Low Reynolds Number Effects in a Ventilated Room. I SSN 1395-7953 R0044 . PAPER NO. 120: P. Lengweiler, P.V. Nielsen, A. Maser, P. Heiselberg , H. Takai: Experimental Method for Measuring Dust Load on Surfaces in Rooms. ISSN 1395-7953 R0045. PAPER NO. 121 : L. Davidson, P.V. Nielsen, C. Topp : Low-Reynolds Number Effects in Ventilated Rooms: A Numerical Study 1395-7953 R0046. PAPER NO. 122: F. Haghighat, H. Brohus, C. Frier, P. Heiselberg: Stochastic Prediction of Ventilation System Performance . ISSN 1395-7953 R0047 . PAPER NO. 123: H. Brohus, F. Haghighat C. Frier, P. Heiselberg: Quantification of Uncertainty in Thermal Building Simulation. Part 1: Stochastic Building Model. ISSN 1395-7953 R0048. PAPER NO. 124: H. Brohus, F. Haghighat C. Frier, P. Heiselberg: Quantification of Uncertainty in Thermal Building Simulation. Part 2: Stochastic Loads. ISSN 1395-7953 R0049. Complete list of papers: http://iee.civi/.auc.dk/i6/publl iee.html ISSN 1395-7953 R0041 Dept. of Building Technology and Structural Engineering Aalborg University, December 2000 Sohngaardsholmsvej 57, DK-9000 Aalborg, Denmark Phone: +45 9635 8080 Fax: +45 9814 8243 http://iee.civil.auc.dk 

Characterization of the Airflow from a Bottom Hung Window under Natural Ventilation

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Characterization of the Airflow from a Bottom Hung Window under Natural Ventilation

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