建筑給排水外文文獻翻譯

1、<p><b>　　本科畢業(yè)設(shè)計</b></p><p><b>　　外文文獻及譯文</b></p><p>　　文獻、資料題目：Sealed building drainage </p><p>　　and vent systems</p><p>　　文獻、資料來源：國道數(shù)據(jù)庫<

2、/p><p>　　文獻、資料發(fā)表（出版）日期：2005.9.12</p><p>　　院 （部）： 市政與環(huán)境工程學(xué)院</p><p>　　專 業(yè)： 給水排水工程</p><p><b>　　班 級： </b></p><p><b>　　姓 名： </b>&l

3、t;/p><p><b>　　學(xué) 號：</b></p><p><b>　　指導(dǎo)教師： </b></p><p>　　翻譯日期： 2012.06</p><p><b>　　外文文獻：</b></p><p>　　Sealed building dra

4、inage and vent systems</p><p>　　—an application of active air pressure transient control and suppression</p><p><b>　　Abstract</b></p><p>　　The introduction of sealed bui

5、lding drainage and vent systems is considered a viable proposition for complex buildings due to the use of active pressure transient control and suppression in the form of air admittance valves and positive air pressure

6、attenuators coupled with the interconnection of the network's vertical stacks. </p><p>　　This paper presents a simulation based on a four-stack network that illustrates flow mechanisms within the pipewor

7、k following both appliance discharge generated, and sewer imposed, transients. This simulation identifies the role of the active air pressure control devices in maintaining system pressures at levels that do not deplete

8、trap seals. </p><p>　　Further simulation exercises would be necessary to provide proof of concept, and it would be advantageous to parallel these with laboratory, and possibly site, trials for validation pur

9、poses. Despite this caution the initial results are highly encouraging and are sufficient to confirm the potential to provide definite benefits in terms of enhanced system security as well as increased reliability and re

10、duced installation and material costs. </p><p>　　Keywords: Active control; Trap retention; Transient propagation </p><p>　　Nomenclature</p><p>　　C+-——characteristic equations </p

11、><p>　　c——wave speed, m/s </p><p>　　D——branch or stack diameter, m </p><p>　　f——friction factor, UK definition via Darcy Δh=4fLu2/2Dg</p><p>　　g——acceleration due to gravi

12、ty, m/s2 </p><p>　　K——loss coefficient </p><p>　　L——pipe length, m </p><p>　　p——air pressure, N/m2 </p><p>　　t——time, s </p><p>　　u——mean air velocity, m/s

13、 </p><p>　　x——distance, m</p><p>　　γ——ratio specific heats </p><p>　　Δh——head loss, m </p><p>　　Δp——pressure difference, N/m2 </p><p>　　Δt——time step, s &l

14、t;/p><p>　　Δx——internodal length, m </p><p>　　ρ——density, kg/m3</p><p>　　Article Outline</p><p>　　Nomenclature </p><p>　　1. Introduction—air pressure transien

15、t control and suppression</p><p>　　2. Mathematical basis for the simulation of transient propagation in multi-stack building drainage networks </p><p>　　3. Role of diversity in system operation

16、</p><p>　　4. Simulation of the operation of a multi-stack sealed building drainage and vent system </p><p>　　5. Simulation sign conventions </p><p>　　6. Water discharge to the netwo

17、rk </p><p>　　7. Surcharge at base of stack 1 </p><p>　　8. Sewer imposed transients </p><p>　　9. Trap seal oscillation and retention </p><p>　　10. Conclusion—viability o

18、f a sealed building drainage and vent system</p><p>　　1.Air pressure transients generated within building drainage and vent systems as a natural consequence of system operation may be responsible for trap se

19、al depletion and cross contamination of habitable space [1]. Traditional modes of trap seal protection, based on the Victorian engineer's obsession with odour exclusion [2], [3] and [4], depend predominantly on passi

20、ve solutions where reliance is placed on cross connections and vertical stacks vented to </p><p>　　atmosphere [5] and [6]. This approach, while both proven and traditional, has inherent weaknesses, including

21、 the remoteness of the vent terminations [7], leading to delays in the arrival of relieving reflections, and the multiplicity of open roof level stack terminations inherent within complex buildings. The complexity of the

22、 vent system required also has significant cost and space implications [8]. </p><p>　　The development of air admittance valves (AAVs) over the past two decades provides the designer with a means of alleviati

23、ng negative transients generated as random appliance discharges contribute to the time dependent water-flow conditions within the system. AAVs represent an active control solution as they respond directly to the local pr

24、essure conditions, opening as pressure falls to allow a relief air inflow and hence limit the pressure excursions experienced by the appliance trap seal [9]. </p><p>　　However, AAVs do not address the proble

25、ms of positive air pressure transient propagation within building drainage and vent systems as a result of intermittent closure of the free airpath through the network or the arrival of positive transients generated remo

26、tely within the sewer system, possibly by some surcharge event downstream—including heavy rainfall in combined sewer applications. </p><p>　　The development of variable volume containment attenuators [10] th

27、at are designed to absorb airflow driven by positive air pressure transients completes the necessary device provision to allow active air pressure transient control and suppression to be introduced into the design of bui

28、lding drainage and vent systems, for both ‘standard’ buildings and those requiring particular attention to be paid to the security implications of multiple roof level open stack terminations. The positive air press</p

29、><p>　　Fig. 1 illustrates both AAV and PAPA devices, note that the waterless sheath trap acts as an AAV under negative line pressure.</p><p>　　Fig. 1. Active air pressure transient suppression devi

30、ces to control both positive and negative surges.</p><p>　　Active air pressure transient suppression and control therefore allows for localized intervention to protect trap seals from both positive and negat

31、ive pressure excursions. This has distinct advantages over the traditional passive approach. The time delay inherent in awaiting the return of a relieving reflection from a vent open to atmosphere is removed and the effe

32、ct of the transient on all the other system traps passed during its propagation is avoided. </p><p>　　2.Mathematical basis for the simulation of transient propagation in multi-stack building drainage network

33、s.</p><p>　　The propagation of air pressure transients within building drainage and vent systems belongs to a well understood family of unsteady flow conditions defined by the St Venant equations of continui

34、ty and momentum, and solvable via a finite difference scheme utilizing the method of characteristics technique. Air pressure transient generation and propagation within the system as a result of air entrainment by the fa

35、lling annular water in the system vertical stacks and the reflection and transmission</p><p>　　Air pressure transient propagation depends upon the rate of change of the system conditions. Increasing annular

36、downflow generates an enhanced entrained airflow and lowers the system pressure. Retarding the entrained airflow generates positive transients. External events may also propagate both positive and negative transients int

37、o the network. </p><p>　　The annular water flow in the ‘wet’ stack entrains an airflow due to the condition of ‘no slip’ established between the annular water and air core surfaces and generates the expected

38、 pressure variation down a vertical stack. Pressure falls from atmospheric above the stack entry due to friction and the effects of drawing air through the water curtains formed at discharging branch junctions. In the lo

39、wer wet stack the pressure recovers to above atmospheric due to the traction forces exerted on the</p><p>　　The application of the method of characteristics to the modelling of unsteady flows was first recog

40、nized in the 1960s [13]. The relationships defined by Jack [14] allows the simulation to model the traction force exerted on the entrained air. Extensive experimental data allowed the definition of a ‘pseudo-friction fac

41、tor’ applicable in the wet stack and operable across the water annular flow/entrained air core interface to allow combined discharge flows and their effect on air entrainment to be </p><p>　　The propagation

42、of air pressure transients in building drainage and vent systems is defined by the St Venant equations of continuity and momentum [9],</p><p>　　These quasi-linear hyperbolic partial differential equations ar

43、e amenable to finite difference solution once transformed via the Method of Characteristics into finite difference relationships, Eqs. (3)–(6), that link conditions at a node one time step in the future to current condit

44、ions at adjacent upstream and downstream nodes, Fig. 2.</p><p>　　Fig.2. St Venant equations of continuity and momentum allow airflow velocity and wave speed to be predicted on an x-t grid as shown. Note , .

45、</p><p>　　For the C+ characteristic:</p><p><b>　　when</b></p><p>　　and the C- characteristic:</p><p><b>　　when</b></p><p>　　where t

46、he wave speed c is given by</p><p>　　These equations involve the air mean flow velocity, u, and the local wave speed, c, due to the interdependence of air pressure and density. Local pressure is calculated a

47、s</p><p>　　Suitable equations link local pressure to airflow or to the interface oscillation of trap seals.</p><p>　　The case of the appliance trap seal is of particular importance. The trap sea

48、l water column oscillates under the action of the applied pressure differential between the transients in the network and the room air pressure. The equation of motion for the U-bend trap seal water column may be written

49、 at any time as</p><p>　　It should be recognized that while the water column may rise on the appliance side, conversely on the system side it can never exceed a datum level drawn at the branch connection.<

50、;/p><p>　　In practical terms trap seals are set at 75 or 50 mm in the UK and other international standards dependent upon appliance type. Trap seal retention is therefore defined as a depth less than the i

51、nitial value. Many standards, recognizing the transient nature of trap seal depletion and the opportunity that exists for re-charge on appliance discharge allow 25% depletion. </p><p>　　The boundary equation

52、 may also be determined by local conditions: the AAV opening and subsequent loss coefficient depends on the local line pressure prediction. </p><p>　　Empirical data identifies the AAV opening pressure, its l

53、oss coefficient during opening and at the fully open condition. Appliance trap seal oscillation is treated as a boundary condition dependent on local pressure. Deflection of the trap seal to allow an airpath to,or from,

54、the appliance or displacement leading to oscillation alone may both be modelled. Reductions in trap seal water mass during the transient interaction must also be included. </p><p>　　3. Role of diversity in s

55、ystem operation</p><p>　　In complex building drainage networks the operation of the system appliances to discharge water to the network, and hence provide the conditions necessary for air entrainment and pre

56、ssure transient propagation, is entirely random. No two systems will be identical in terms of their usage at any time. This diversity of operation implies that inter-stack venting paths will be established if the individ

57、ual stacks within a complex building network are themselves interconnected. It is proposed that th</p><p>　　In order to fully implement a sealed building drainage and vent system it would be necessary for th

58、e negative transients to be alleviated by drawing air into the network from a secure space and not from the external atmosphere. This may be achieved by the use of air admittance valves or at a predetermined location wit

59、hin the building, for example an accessible loft space. </p><p>　　Similarly, it would be necessary to attenuate positive air pressure transients by means of PAPA devices. Initially it might be considered tha

60、t this would be problematic as positive pressure could build within the PAPA installations and therefore negate their ability to absorb transient airflows. This may again be avoided by linking the vertical stacks in a co

61、mplex building and utilizing the diversity of use inherent in building drainage systems as this will ensure that PAPA pressures are themsel</p><p>　　Diversity also protects the proposed sealed system from se

62、wer driven overpressure and positive transients. A complex building will be interconnected to the main sewer network via a number of connecting smaller bore drains. Adverse pressure conditions will be distributed and the

63、 network interconnection will continue to provide venting routes. </p><p>　　These concepts will be demonstrated by a multi-stack network.</p><p>　　4. Simulation of the operation of a multi-stack

64、 sealed building drainage and vent system</p><p>　　Fig. 3 illustrates a four-stack network. The four stacks are linked at high level by a manifold leading to a PAPA and AAV installation. Water downflows in a

65、ny stack generate negative transients that deflate the PAPA and open the AAV to provide an airflow into the network and out to the sewer system. Positive pressure generated by either stack surcharge or sewer transients a

66、re attenuated by the PAPA and by the diversity of use that allows one stack-to-sewer route to act as a relief route for the </p><p>　　The network illustrated has an overall height of 12m. Pressure transients

67、 generated within the network will propagate at the acoustic velocity in air . This implies pipe periods, from stack base to PAPA of approximately 0.08s and from stack base to stack base of approximately 0.15s. </p>

68、;<p>　　In order to simplify the output from the simulation no local trap seal protection is included—for example the traps could be fitted with either or both an AAV and PAPA as examples of active control. Traditi

69、onal networks would of course include passive venting where separate vent stacks would be provided to atmosphere, however a sealed building would dispense with this venting arrangement.</p><p>　　Fig.3.Four s

70、tack building drainage and vent system to demonstrate the viability of a sealed building system.</p><p>　　Ideally the four sewer connections shown should be to separate collection drains so that </p>

71、<p>　　diversity in the sewer network also acts to aid system self venting. In a complex building this requirement would not be arduous and would in all probability be the norm. It is envisaged </p><p>　

72、　that the stack connections to the sewer network would be distributed and would be to a below ground drainage network that increased in diameter downstream. Other connections to the </p><p>　　network would i

73、n all probability be from buildings that included the more traditional open vent system design so that a further level of diversity is added to offset any downstream sewer surcharge events of long duration. Similar consi

74、derations led to the current design guidance for dwellings. </p><p>　　It is stressed that the network illustrated is representative of complex building drainage networks. The simulation will allow a range of

75、 appliance discharge and sewer imposed transient conditions to be investigated. </p><p>　　The following appliance discharges and imposed sewer transients are considered: </p><p>　　1. w.c. discha

76、rge to stacks 1–3 over a period 1–6s and a separate w.c. discharge to stack 4 between 2 and 7s.</p><p>　　2. A minimum water flow in each stack continues throughout the simulation, set at 0.1L/s, to represent

77、 trailing water following earlier multiple appliance discharges.</p><p>　　3. A 1s duration stack base surcharge event is assumed to occur in stack 1 at 2.5s.</p><p>　　4. Sequential sewer transie

78、nts imposed at the base of each stack in turn for 1.5s from 12 to 18s.</p><p>　　The simulation will demonstrate the efficacy of both the concept of active surge control and inter-stack venting in enabling th

79、e system to be sealed, i.e. to have no high level roof penetrations and no vent stacks open to atmosphere outside the building envelope. </p><p>　　The imposed water flows within the network are based on ‘rea

80、l’ system values, being representative of current w.c. discharge characteristics in terms of peak flow, 2l/s, overall volume, 6l, and duration, 6s. The sewer transients at 30mm water gauge are representative but not exce

81、ssive. Table 1 defines the w.c. discharge and sewer pressure profiles assumed. </p><p>　　Table1. w.c. discharge and imposed sewer pressure characteristics </p><p>　　5. Simulation conventions<

82、/p><p>　　It should be noted that heights for the system stacks are measured positive upwards from the stack base in each case. This implies that entrained airflow towards the stack base is negative. Airflow ent

83、ering the network from any AAVs installed will therefore be indicated as negative. Airflow exiting the network to the sewer connection will be negative. </p><p>　　Airflow entering the network from the sewer

84、connection or induced to flow up any stack will be positive. </p><p>　　Water downflow in a vertical is however regarded as positive. </p><p>　　Observing these conventions will allow the followin

85、g simulation to be better understood. </p><p>　　6. Water discharge to the network</p><p>　　Table 1 illustrates the w.c. discharges described above, simultaneous from 1s to stacks 1–3 and from 2s

86、 to stack 4. A base of stack surcharge is assumed in stack 1 from 2.5 to 3s. As a result it will be seen from Fig. 4 that entrained air downflows are established in pipes 1, 6 and 14 as expected. However, the entrained a

87、irflow in pipe 19 is into the network from the sewer. Initially, as there is only a trickle water flow in pipe 19, the entrained airflow in pipe 19 due to the w.c. discharges al</p><p>　　Fig.4.Entrained airf

88、lows during appliance discharge.</p><p>　　Following the w.c. discharge to stack 4 that establishes a water downflow in pipe 19 from 2 s onwards, the reversed airflow initially established diminishes due

89、 to the traction applied by the falling water film in that pipe. However, the suction pressures developed in the other three stacks still results in a continuing but reduced reversed airflow in pipe 19. As the water down

90、flow in pipe 19 reaches its maximum value from 3 s onwards, the AAV on pipe 12 opens fully and an increased airflow from</p><p>　　Fig. 5 illustrates the air pressure profile from the stack base in both

91、stacks 1 and 4 at 2.5 s into the simulation. The air pressure in stack 4 demonstrates a pressure gradient compatible with the reversed airflow mentioned above. The air pressure profile in stack 1 is typical for a st

92、ack carrying an annular water downflow and demonstrates the establishment of a positive backpressure due to the water curtain at the base of the stack.</p><p>　　Fig.5.Air pressure profile in stacks 1 and 4 i

93、llustrating the pressure gradient driving the reversed airflow in pipe 19. </p><p>　　The initial collapsed volume of the PAPA installed on pipe 13 was 0.4l, with a fully expanded volume of 40l, however due t

94、o its small initial volume it may be regarded as collapsed during this phase of the simulation. </p><p>　　7. Surcharge at base of stack 1</p><p>　　Fig. 6 indicates a surcharge at the base of sta

95、ck 1, pipe 1 from 2.5 to 3 s. The entrained airflow in pipe 1 reduces to zero at the stack base and a pressure transient is generated within that stack, Fig. 6. The impact of this transient will also be seen later i

96、n a discussion of the trap seal responses for the network.</p><p>　　Fig.6.Air pressure levels within the network during the w.c. discharge phase of the simulation. Note surcharge at base stack 1, pipe 1 at 2

97、.5s. </p><p>　　It will also be seen, Fig. 6, that the predicted pressure at the base of pipes 1, 6 and 14, in the absence of surcharge, conform to that normally expected, namely a small positive back pressur

98、e as the entrained air is forced through the water curtain at the base of the stack and into the sewer. In the case of stack 4, pipe 19, the reversed airflow drawn into the stack demonstrates a pressure drop as it traver

99、ses the water curtain present at that stack base. </p><p>　　The simulation allows the air pressure profiles up stack 1 to be modelled during,and following, the surcharge illustrated in Fig. 6. Fig. 7(a) and

100、(b) illustrate the air pressure profiles in the stack from 2.0 to 3.0 s, the increasing and decreasing phases of the transient propagation being presented sequentially. The traces illustrate the propagation of the p