Advances in WaterBased Fire Suppression Modeling: - PowerPoint PPT Presentation

1 / 26
About This Presentation
Title:

Advances in WaterBased Fire Suppression Modeling:

Description:

Physical models characterizing the break-up process and the ... SHADOWGRAPH / PTV. BREAKUP IMAGING. DROP SIZE / VELOCITY. 24 of 26. Experimental Plans ... – PowerPoint PPT presentation

Number of Views:49
Avg rating:3.0/5.0
Slides: 27
Provided by: andrema
Category:

less

Transcript and Presenter's Notes

Title: Advances in WaterBased Fire Suppression Modeling:


1
Advances in Water-Based Fire Suppression
Modeling Evaluating Sprinkler Discharge
Characteristics
June 24, 2008
7th International Fire Sprinkler Conference and
Exhibition Copenhagen, Denmark Students Ning
Ren, Andrew Blum, Di Wu, and Chi Do Faculty
Advisor Andre Marshall Sponsors NFSA, FM
Global, NSF
2
Overview
  • Introduction
  • Motivation
  • Project History
  • Previous Work
  • Global Objective
  • Evaluate Discharge Characteristics
  • Advanced Measurements
  • SAM Development
  • Approach
  • Experimental
  • Modeling (SAM)
  • Results
  • Sheet Formation (Deflector)
  • Sheet Breakup
  • Drop Formation
  • Dispersion
  • Summary
  • Plans
  • Experimental
  • Modeling

3
Motivation
Gain New Knowledge
  • Physical models characterizing the break-up
    process and the associated initial spray in fire
    suppression devices have yet to be developed.

Develop Injector Technology
  • The absence of this analytical capability impedes
    the development of fire suppression
    injectors/systems.

Understanding the relationship between
atomization physics and injector control
parameters would facilitate a transition away
from cut and try injector development.
4
Motivation
D
inlet
L
inlet
D
o
L
jet
A
A
?
boss
Section A-A
D
boss
t
?
tine
arm
?
space
D
def
Characterization
Cut and Try
5
Motivation
Advance Fire Protection Engineering Practices
  • CFD modeling tools of fire phenomena are becoming
    increasingly popular for fire protection analysis
    and performance based design.
  • The absence of physical models describing
    atomization in sprinklers and water mist
    injectors results in uncertainties in CFD
    simulation of suppressed fires.
  • Errors in the specification of the initial spray
    will be propagated and amplified during
    dispersion calculations.

The atomization model represents a critical
missing link in the modeling of suppressed fires.
6
Project History
UM Fire Suppression Spray Research
FY2005
FY2006
FY2007
FY2008
FY2009
FY2012
FY2010
FY2011
NFSA
Sprinkler Atomization Modeling and FDS Integration
Betatti - U. Modena
DuPont
Surfactant Effects on Fire Suppression
HP Mist Modeling
FM Global
Scaling Laws and Models for Fire Suppression
Devices
NSF CAREER Award Exploring Atomization and Jet
Fragmentation in Combustion and Fire Suppression
Systems
7
Previous Work
Previous Research
1
3
FD
Fs
8
Global Objective
Evaluate discharge characteristics from fire
suppression devices using measurements and models.
  • Parameter Space
  • based on varied injector geometry and injection
    conditions.
  • Experiments
  • based on state-of-the art diagnostics focused on
    the initial spray.
  • Analysis
  • based on physics based models using
    semi-empirical approaches (e.g. scaling laws and
    wave dispersion analysis).

9
Approach
Injected Flow
Injectors

J
e
t

TYCO TY4211
Gr
ow
t
h

o
f

W
a
v
e
s

D
e
f
le
ct
o
r

LP Nozzle 2 bar 700 ?m
Sh
e
e
t


F
or
m
a
t
io
n

TYCO AM4
Sh
e
e
t

L
igamen
t


?
Li
g
a
m
e
nt

Dr
o
p


?
MP Nozzle 15 bar 225 ?m
HP Nozzle 100 bar 60 ?m
10
Approach
Geometric parameter space w/n LP injector
(sprinkler) configuration
3.2, 6.7, 9.7 mm
38 mm
Basis Nozzle
Sprinkler
11
Approach
Trajectory Measurements (PLIF)
Camera FOV
texp 900 ?s
Cooke 16-bit cooled 2.0Mpixel High-Speed Digital
Video Camera.
12
Approach
Sheet Break-up Measurements
13
Approach
Drop Size Measurements
Malvern Spraytec Analyzer (Light Diffraction
Technique)
Local Measurements
Local Drop Size Distribution
P 2.07 bar r/R 0.45
Local
14
Approach
Volume Flux Measurements
BasisDo 9.7 mm P 2.07 bar
BasisDo 9.7 mmP 2.07 bar
3.0 m
1.0 m
1.0 m
dv50 780 µm
15
Approach
Radius where Wall Effects Reach Free Surface
Impinging Jet (Watson, 1964)
Viscous interactions with deflector important for
initial thickness and velocity of unstable free
liquid sheet.
Jet Radius
Deflector Radius
Arbitrary Length Scale Determined from Matching
Kinematic Viscosity
Jet Flow Rate
Annular Sheets (Ibrahim, 2004)
Transport equations for mass and momentum provide
the sheet trajectory.
16
Approach
Dimensionless Wave Growth Rate
Viscous
Inviscid
Fastest Growing Wave
Most Unstable Wavelength
Gas
p-
p-
p-
U
p
p
Sinusoidal Waves
Viscous
Wave Growth (Sterling and Sleicher, 1975 Weber,
1931)
r
The most unstable wave is determined, which
breaks up the sheet at rbu,lig into a fragment
having characteristic length ?bu,lig.
r
Vjet
z
p
p-
17
Results
Sheet Formation
Governing Equations
, b
Dimensionless Solution
  • The thickness and velocity of the sheet is
    reduced by viscous effects depending on the
    nozzle geometry (not yet accounting for spaces).

18
Results
Sheet Formation
  • Two distinct streams are formed the jet is
    deflected radially outward along the tines and
    the jet is forced downward through the spaces
  • The flow split between these streams governs the
    sheet thickness and the resulting drop size.

19
Results
Sheet Breakup
Standard Nozzle, Do 6.35 mm, p 2 bar
  • Sheet breakup locations occur several jet
    diameters away from the sprinkler.
  • Data collapses well with appropriate theory

20
Results
Drop Formation
p 2 bar
  • Drop size in the space stream are siginificantly
    smaller than tine stream, but follow
    Rosin-Rammler
  • Testing scaling law for drop size

21
Results
Dispersion
The radial coordinate has been normalized with
the maximum theoretical radial value for each
condition.
Spatial Drop Size Distributions
Spatial Volume Flux Distributions
K 7.2 (0.5)
K 25.9 (1.8)
K 54.7 (3.4)
22
Summary
  • Viscous effects along the deflector can be
    important (for small K-factors).
  • Two well characterized sheets (radially expanding
    and orthogonal fan) are formed through the tines
    and the spaces.
  • SAM successfully models the tine stream. Space
    stream submodel in SAM currently under
    development.
  • Sheet breakup locations are predicted well by SAM
    with We-1/3.
  • Ligament break-up (high We) modes and rim
    break-up modes (low We) are observed. The We
    transition depends on nozzle geometry.
  • Drop size predicted well by SAM when nozzle
    operates in ligament breakup mode with We-1/3.

23
Experimental Plans
BREAKUP IMAGING
Tine Stream
Space Stream
QUANTITATIVE SHADOWGRAPH / PTV
DROP SIZE / VELOCITY
24
Experimental Plans
25
SAM Modeling Plans
Device Characterization
Space Stream Submodel
Fundamental Models
To Outer
Splitter
To Inner
Expanding Validated Parameter Space
CFD Integration
Standard Nozzle(Tyco D3 Nozzle)
Basis Nozzle
26
Questions?
Write a Comment
User Comments (0)
About PowerShow.com