Title: Fundamental Ice Crystal Accretion Physics Studies
1Fundamental Ice Crystal Accretion Physics Studies
- Peter Struk, Paul Tsao, Mario Vargas
- NASA Glenn Research Center
- Tom Currie, Dan Fuleki, Danny Knezevici
- National Research Council of Canada
- with additional sponsorship by
- Federal Aviation Administration
- Transport Canada
2Ice-Crystal Icing Aspects
- Atmospheric Characterization
- Particle size distributions, morphology
- Concentrations
- Where specifically in the engine could
ice-crystal icing occur? - Internal conditions?
- Changes to particle size due to impact with
rotating blades? - Concentrations as flow area changes?
- Mixed phase conditions?
Graphic NASA (www.ueet.nasa.gov)
- We need to understand the conditions leading to
ice-crystal icing. - Can we simulate these conditions in an
experimental facility to better understand the
fundamental aspects of ice-crystal icing?
3Previous Studies
- Ice Crystal Testing on a Flat Plate (MacLeod
2007) - Demonstrated rapid ice buildup on a heated plate
with stagnation blocks exposed to ice crystals. - Ice appeared to not adhere but rather was held
against the stagnation point until it grew larger
and shed due to aerodynamic forces. - Mixed-phase ice-crystal testing on an airfoil
in a S-duct (Mason, Chow, Fuleki, 2010) - Demonstrated that ice can form on the airfoil and
other surfaces of the S-duct at air temperatures
significantly warmer than freezing.
Images NRC, with permission
4Fundamental Ice Crystal Accretion Studies
- Subject to operating limits of the facility,
focus on conditions representative of those found
in a low pressure compressor - Research Approach
- Simple test geometry (i.e. wedge airfoil)
- Utilizes NRC Research Altitude Test Facility
(RATFac) - Can inject ice crystals into a warm environment
from near SL to 30,000 ft. - Test over a range of conditions
- Identify study parameters governing accretion
initiation growth - Document time evolution of ice accretions -
initiation, growth, shedding - Summary of testing to date (2 entries)
- Nov. 2010 focused on identifying onset
conditions for ice-crystal accretion - Began to establish the envelope bounding the
onset of accretion events - Noticed that the temperature, altitude and
humidity all could play a role - Mar. 2011 further investigated combined effect
of temperature, altitude, and humidity (i.e. the
air wet bulb temperature or TWB) on the onset and
growth rate of ice crystal accretion
5Wedge Airfoil in RATFac Cascade Tunnel
Dimensions mm
Top view (normal to icing surface)
Connection to exhauster
Rectangular inlet bellmouth
Airfoil
Large front window
Side view (end view of leading edge)
Graphics NRC, with permission
6Wedge Airfoil Test Conditions Results
- Conditions
- Mach number 0.2?0.4 (primarily 0.2 0.25)
- Total pressure 6.5 and 13.5 psia
- Injected IWCi 0 ? 20 g/m3
- Supplemental LWCi 0 ? 3 g/m3
- Total air temperature 5 ? 23C
- Ice MMD 90-200µ (estimated)
- Water MVD 40µ
- IWC, LWC measured with SEA multi-element probe
150mm upstream of airfoil? IWCm , LWCm
- Preliminary results showed there are two types of
ice accretion - Ice accumulates and is very slushy with frequent
shedding when - evaporation cooling is weak, i.e. TWB gt 0?C
- 2. Ice accretion is firm and little shedding when
evaporation cooling is strong, i.e. TWB lt 0C.
7Slushy Ice Accumulation with Frequent Shedding
Video shown at 8x real time
Run 522 IWCi, LWCi(17,0.5) g/m3, 6.5psia,
M0.25, To20C, RH 13, TWB 2.7C
Video NASA
8Firm Ice Accretion with Little Shedding
Video shown at 8x real time
Run 543, IWCi, LWCi (7,1.5) g/m3, 6.5psia,
M0.25, To13C, RH8, TWB-2C
Video NASA
9Energy Balance to Better Understand Physics
- Convection to / from air
- Conduction to / from solid
- Water Flow In
- Surface Flow
- Impinging water mass
- ice, water, mixed phase
- Freezing or melting
- Water Flow Out
- Surface Run Back
- Bounce / Splash
- Erosion / shed
- Evaporation/Sublimation
IWC, LWC
Tsurf
U T P
Control volume on icing surface
PW?
Graphic NASA
10Wet Bulb Temperature
- TWB ? balance convection with evaporative cooling
and no conduction to solid - Wetted surface evaporates cools down
- Convection provides energy to surface
- Surface temperature can approach TWB in these
idealized conditions -
- The wet bulb temperature represents the humid air
energy transfer (function of T, P, Pw) - Lower humidity or lower pressure ? more
evaporative cooling lower TWB
IWC, LWC
Tsurf
U T P
no conduction
Control volume on icing surface
PW?
Graphic NASA
TWB helped us identify onset of one type of ice
accretion (not complete answer to identifying all
ice accretion conditions)
11Planned Future Work
- Scaling work to include ice-crystal and mixed
phase conditions - Identify scaling parameters that govern the ice
crystal accretion process - Multi-wire probe characterization in mixed phase
conditions (Apr. 2012) - Addition of imaging upstream of probe
- Investigate pooling in multi-wire probe
- Develop melt-ratio correlation for ice-crystals
scaling condition calculation - NACA0012 airfoil experiments to validate scaling
methods (Dec. 2012) - Measuring ice shape profile along mid-span of
model - Addition of heater tape along model root and rip
Heater Tape
132 mm
Thermocouples (13)
12Challenges in Ice Crystal Icing Research
- Can be broadly summarized in these categories
- Understanding generating internal-to-engine
environmental conditions - Measuring conditions
- Ice accretion measurements
- Understanding physics
13Challenge Understanding Simulating Environment
- Are the conditions we are simulating relevant to
a LPC? - Pressures (6.5 13.5 psia)
- Temperatures (TAT gt 0 to 20?C)
- Mach numbers (0.2 ? 0.4)
- Ice crystal / mixed phase characteristics
- Size distribution (90-200 µm MMD)
- Particle thermal phase distribution (not well
understood) - We need to know the above conditions in an
internal engine environment. - Can we effectively generate these conditions ?
- Injecting ice into warm environment is difficult
- Uniformity of conditions?
- Importance of heated or cooled surfaces?
14Challenge Measuring Conditions
- Phase of particles
- Can be fully glaciated, fully melted, partially
melted - Using hot-wire technique (SEA multi-wire)
- Needs known calibration source (okay for LWC
alone) - Under-reads IWC and LWC in mixed-phase, possible
pooling _at_ high IWC - Temperature of particles
- Unknown but important to accurately model physics
- Not likely the same temperature as environment in
ice-crystal engine icing - Particle size distributions (see next slides)
- Small particles moving at high velocities
- Using imaging methods
- Need good resolution stop-action capability
- Work underway using backlit laser sheet methods
SEA Multi-wire Probe
Image NASA
All Vapor Out
Graphic NASA
15Challenge Ice Shape Measurement (1 of 2)
- Ice shape and morphology required to compare to
simulations - Traditional methods (tracings castings) not
easily adaptable - NASA developed technique to measure leading edge
ice growth (1D) from images (Struk, et al. 2012).
Clean Airfoil
ROI 1
ROI 11
Asymmetric ice growth (test 515)
Images NASA
16Challenge Ice Shape Measurement (2 of 2)
- 2D 3D Ice Shape Profiles from images desired
- Preliminary work underway
Far wall accumulation profile (outer white)
Near wall accumulation profile (outer white)
Mid-plane profile (inner white)
Heater tape to prevent ice accumulation near
endwall
Images NASA
17Summary
- Fundamental ice-crystal accretion physics studies
underway - Demonstrated that ice accretions can occur when
ice-crystals are injected onto an airfoil in warm
conditions. - Observed ice accretion is firm and little
shedding when evaporation cooling is strong, i.e.
TWB lt 0C. - Ice accumulates and is very slushy with frequent
shedding when evaporation cooling is weak, i.e.
TWB gt 0C - TWB may be able to help identify locations
susceptible to icing - However, it is not the complete answer (i.e.
LWC/TWC ratio, others?) - Challenges exist for fundamental experiments
- Understanding generating internal-to-engine
environmental conditions - Measuring conditions
- Ice accretion measurements
- Understanding physics