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| Fältnamn | Indikatorer | Metadata |
|---|---|---|
| 000 | 05206nam a2200445 4500 | |
| 001 | oai:DiVA.org:hig-17832 | |
| 003 | SwePub | |
| 008 | 141109s1996 | |||||||||||000 ||eng| | |
| 020 | a 9171706674q print | |
| 024 | 7 | a https://urn.kb.se/resolve?urn=urn:nbn:se:hig:diva-178322 URI |
| 040 | a (SwePub)hig | |
| 041 | a engb eng | |
| 042 | 9 SwePub | |
| 072 | 7 | a vet2 swepub-contenttype |
| 072 | 7 | a dok2 swepub-publicationtype |
| 100 | 1 | a Karimipanah, Taghi,d 1953-u Högskolan i Gävle,Avdelningen för bygg- energi- och miljöteknik4 aut0 (Swepub:hig)tkh |
| 245 | 1 0 | a Turbulent jets in confined spaces :b application in mixing ventilation: experimental and numerical studies |
| 264 | 1 | a Stockholm :b KTH Royal Institute of Technology,c 1996 |
| 300 | a 95 s. | |
| 338 | a electronic2 rdacarrier | |
| 520 | a The basis of mixing ventilation is the airflow supply to the room by means of jets initiatedfrom the ventilation diffusers. To avoid the draught problem, the design of mixing ventilationmakes uses the throw term, which is defined as the distance to the supply air terminal inwhich the jet centreline mean velocity is decreased to a given value. Traditionally, the throw ismeasured by the supply air device manufacturer. The throw is applied by designers to estimatethe velocity levels in the occupied zone. A standard for determining the throw is the CENstandard CEN/TC156/WG4 N86 "Draft Standard. Air terminal Devices. AerodynamicsTesting And Rating For Mixed Flow Application".The measurement of the throw is very time consuming even with the free jets and theinfluence of the room (the effect of confinement) is not considered. The objective of thepresent study is to give a basis for modifying the existing design and testing method used topredict the velocities in the occupied zone during the design process. A new method whichmay probably be more easier than the existing methods and at the same time give a betterprecision by including the confinement effect.In this thesis two methodological systems of experiment and numerical simulations have beenused. The numerical predictions are used in comparison with the measurements. Thereasonable agreement of the above mentioned methods is implemented to numerical study ofthe other room configurations which are not experimentally studied. This examining methodallows the possibility of studying a lot of configurations and in this manner generalising of theresults. Although the experimental part was made for both model-scale and full-scale testrooms, a large amount of data was obtained for a new test room whose dimension aresystematically varied. All of studies have been made for the isothermal case and themeasurements of velocities and pressures conducted along the room perimeters. The effect ofshort and deep rooms on the properties of the jet ( velocities, pressure, integral scale, jetmomentum, the rate of spreading of jet and turbulence intensities) have been carried out.Some old and recent investigations have been examined. Specially the concept of correlationsfrom open to closed rooms is criticised. It is also shown that the flow field in a confined roomis affected by many other factors than the Reynolds number. The surface pressure on theperimeters was used to calculate the reaction forces at the corners which causes recirculatingbubbles at corners. A study of the turbulent axisymmetric jet which is the basic element inturbulent shear flows and some restrictions of the traditional measurement techniques at theregion of interest in ventilation applications are discussed. The jet momentum is measured byweighing on a balance. Also a study of jets which collide with a wall , that is impinging jet,the effect of walls and confinement on the jet momentum have experimentally andnumerically been carried out. A new momentum balance model was developed for both thefree jet and confined one. An empirical relation has been found for estimation of the room’srotation centre which is used for validation of CFD results.Finally, it is found that the jets in a ventilated room which are a combination of free jet, walljet and impinging jet differ from the traditional wall jets. The rate of spreading of the jet andthe maximum velocity decay in a ventilated room are also different depending on the roomsize and its confinement. | |
| 650 | 7 | a TEKNIK OCH TEKNOLOGIERx Annan teknik0 (SwePub)2112 hsv//swe |
| 650 | 7 | a ENGINEERING AND TECHNOLOGYx Other Engineering and Technologies0 (SwePub)2112 hsv//eng |
| 653 | a turbulent | |
| 653 | a wall jet | |
| 653 | a impinging jet | |
| 653 | a free jet | |
| 653 | a confinement effect | |
| 653 | a pressure | |
| 653 | a throw | |
| 653 | a experimental | |
| 653 | a numerical | |
| 653 | a corner | |
| 653 | a momentum | |
| 653 | a mixing ventilation | |
| 700 | 1 | a Sandberg, Mats4 ths |
| 700 | 1 | a Awbi, H. A.,c Professoru University of Reading, England4 opn |
| 710 | 2 | a Högskolan i Gävleb Avdelningen för bygg- energi- och miljöteknik4 org |
| 856 | 4 | u https://hig.diva-portal.org/smash/get/diva2:761872/FULLTEXT01.pdfx primaryx Raw objecty fulltext |
| 856 | 4 8 | u https://urn.kb.se/resolve?urn=urn:nbn:se:hig:diva-17832 |
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