Enclosure Thermal Control 25 August 2003 ATST CoDR Dr. Nathan Dalrymple Air Force Research Laboratory Space Vehicles Directorate.

Slides:



Advertisements
Similar presentations
Starter Question If you touch two objects that are the same temperature, why would one feel colder than the other?
Advertisements

Energy Efficient Heating Ventilating and Air Conditioning.
Extra Large Telescope Wind Engineering. Wind and Large Optical Telescopes Wind is a key factor in the design of large telescopes: larger wind-induced.
Conduction Conceptests
HEAT LOSS & HEAT GAIN HEAT FLOW. Heat flows from high temperature to low temperature There are 3 types/methods of heat flow/transfer: 1.Conduction- through.
Five star hotel in Nablus
HVAC System Design PES Institute of Technology. Objective Goal: To develop an automotive air-conditioning system that is smaller and lighter than with.
HVAC: heating, ventilating, and air conditioning this is a thermostat: it sends signals to the heating/cooling system.
Coupling a Network HVAC Model to a Computational Fluid Dynamics Model Using Large Eddy Simulation Jason Floyd Hughes Associates, Inc Fire + Evacuation.
So Far: Conservation of Mass and Energy Pressure Drop in Pipes Flow Measurement Instruments Flow Control (Valves) Types of Pumps and Pump Sizing This Week:
ATA Melbourne Branch presentation April 2008 Jim Lambert
Mauna Kea. The Gemini Project Who: An international partnership of the United States, United Kingdom, Canada, Chile, Argentina, Brazil and Australia.
TopDrive: RP3 Thermal Management of Battery Module Unit of Electronics Integration and Reliability Department of Electronics.
Energy in Focus Energy Savings with Water Based Systems By Maija Virta Specialist of Indoor Environment Technology.
The Heat Stop 25 August 2003 ATST CoDR Dr. Nathan Dalrymple Air Force Research Laboratory Space Vehicles Directorate.
Example 1:- An annular alloyed aluminum (k = 180 W/m . K ) fin of rectangular profile is attached to the outer surface of a circular tube having an outside.
Physics 52 - Heat and Optics Dr. Joseph F. Becker Physics Department San Jose State University © 2003 J. F. Becker.
COMMERCIAL REFRIGERATION
 Install new air cooled high efficiency screw chiller (variable speed)  Install new fan coils with ECM motors and low temperature heating coils and proper.
Cooling Update (May 2011) Tim. Overview From last time – Estimate Power Loads Active components Extraneous heat sources – Develop methodology for exploring.
1 HVAC OVERVIEW and VALUE ENGINEERING ITEMS August 13, 2008 CLIC Working Group CES Lee Hammond, Fermilab.
Value Engineering Session Air Treatment / HVAC November 27, 2007 Lee Hammond, FNAL CFS.
Page 1 AO in AO A daptive O ptics in A stronomical O bservations Diana R. Constantin ASTRONOMICAL INSTITUTE OF THE ROMANIAN ACADEMY.
Objective Heat Exchangers Learn about different types
HEAT EXCHANGER.
Heat Transfer Equations For “thin walled” tubes, A i = A o.
DESIGN AND PERFORMANCE EVALUATION OF AN EVAPORATIVE HEAT EXCHANGER A.O. MURITALA, S.O. OBAYOPO, S.K. FASHOGBON, O.T. POPOOLA*, S.A ADIO Department of Mechanical.
M2 and Transfer Optics Thermal Control 25 August 2003 ATST CoDR Dr. Nathan Dalrymple Air Force Research Laboratory Space Vehicles Directorate.
Utilities 14 October 2008 Martin Nordby, Gordon Bowden.
Viewing the Universe through distorted lenses: Adaptive optics in astronomy Steven Beckwith Space Telescope Science Institute & JHU.
BDS Magnet-Power System-Facility Optimization1 ILC BDS Kickoff Meeting Basis for Magnet, Power System and Cooling Facility Optimization Discussion Paul.
Woodstoves 1 Woodstoves. Woodstoves 2 Introductory Question Which is more effective at heating a room: Which is more effective at heating a room: A. a.
Chapter Woodstoves.
Senior Design Team #18 Lacey Ednoff Brianna Beconovich Jarimy Passmore Jesse Poorman.
Thermal Physics Modes of Heat Transfer.
4/12/2011Controller Cooling Test1 Array Controller Cooling Test Bill Hoffmann April 12, 2011 This is a report on a test of the chilled water-to-air heat.
LHC Phase II Collimator Compact jaw simulations New FLUKA => ANSYS mapping scheme New 136mm x 950mm jaw –60cm primary collimator –Helical cooling channel.
So Far: Conservation of Mass and Energy Pressure Drop in Pipes Flow Measurement Instruments Flow Control (Valves) Types of Pumps and Pump Sizing This Week:
1 ISAT Module III: Building Energy Efficiency Topic 7: Transient Heating and Air Conditioning Loads  Thermal Admittance  Intermittent Heating 
Heat Transfer Carlos Silva December 9 th Energy transference Energy can be transferred between a system and its surroundings Work Heat Mass flow.
NuMI NuMI Target Hall Air System Review Introduction July 30, 2003 Jim Hylen / FNAL Page 1 NuMI Target Hall Air System Review Introduction Air system for.
M1 Thermal Control 25 August 2003 ATST CoDR Dr. Nathan Dalrymple Air Force Research Laboratory Space Vehicles Directorate.
Full Scale Thermosyphon Design Parameters and Technical Description Jose Botelho Direito EN/CV/DC 19 November, th Thermosyphon Workshop.
Heat Transfer Equations. Fouling Layers of dirt, particles, biological growth, etc. effect resistance to heat transfer We cannot predict fouling factors.
Adaptive Optics in the VLT and ELT era Atmospheric Turbulence
Sherril Soman Grand Valley State University Lecture Presentation Chapter 6-2 Thermochemistry.
Get with a partner and go over your solutions to the 3G and 3F Test Review. Pay particular attention to #9 on the Fluid Technology side. You have ~12 minutes.
Heat Transfer Equations For “thin walled” tubes, A i = A o.
Mount and Coudé Lab Thermal Control 25 August 2003 ATST CoDR Dr. Nathan Dalrymple Air Force Research Laboratory Space Vehicles Directorate.
NCSX VACUUM VESSEL HEATING/COOLING PL Goranson Final Design Review April 4, 2006 Coolant Hose Assemblies and Thermo- hydraulics NCSX.
Cooling System Get the engine up to optimum operating Temperature as quickly as possible and maintains it at that temperature. Controls the heat produced.
Chapter 15 Heat Transfer. Second Law of Thermodynamics Heat flows naturally from hot to cold objects. Heat will not flow spontaneously from cold object.
1 | WEATHERIZATION ASSISTANCE PROGRAM STANDARDIZED CURRICULUM – August 2010eere.energy.gov Moisture Assessment WEATHERIZATION ENERGY AUDITOR SINGLE FAMILY.
The Blanco Environmental Control System Alistair R. Walker November
NUMERICAL SIMULATIONS OF AIRFLOW THROUGH 8m ENCLOSURES
Conservation of Mass and Energy
HEAT EXCHANGER.
Lesson 24 NATURAL CIRCULATION
12: Greenhouses and the Earth System
Bell work Predict whether leaving the refrigerator door open on a hot summer day will help to cool the kitchen.
CHAPTER 3 VENTILATION.
CFHT is hot! (and cold) Kevin Ho, Derrick Salmon, Steve Bauman
PES 1000 – Physics in Everyday Life
Summary of Gemini Technical Report No. 1
Comparison of heat loss with a wetsuit vs. without
AVE stands for Atmospheric Vortex Engine.
Comments on P. Hickson “TMT image quality at Mauna Kea and La Palma”
ATA Melbourne Branch presentation April 2008 Jim Lambert
Presentation transcript:

Enclosure Thermal Control 25 August 2003 ATST CoDR Dr. Nathan Dalrymple Air Force Research Laboratory Space Vehicles Directorate

Enclosure Thermal Control Function: Suppress seeing If a surface is the same temperature as the surrounding air, that surface introduces no seeing Seeing is caused by temperature differences

Requirements 1.Suppress enclosure seeing a.Racine experiment:  = 0.15  T i - T e ) 1.2 b.Ford analysis:  =  T s - T e  1.2 c.IR HB aerodynamic analysis:  =  T  V,  d.Bottom line: requirements on surface-air  T, interior- exterior  T, and wind flushing 2.Provide passive interior flushing to equalize interior and exterior temperatures and to suppress structure and mirror seeing Ref: Racine, Rene, “Mirror, dome, and natural seeing at CFHT,” PASP, v. 103, p. 1020, 1991.

Error Budgets (nm) Exterior budgetInterior budget nm10 nm arcsec0.02 arcsec arcsec0.025 arcsec

IR Handbook Seeing Analysis Given layer thickness and  T, we can estimate . Wavefront variance Gladstone-Dale parameter Fluctuating densityLine-of-sight correlation length Layer thickness Phase variance Surface-air temperature difference Blur angle Strong/weak cutoff ~ 2 rad Ref: Gilbert, Keith G., Otten, L. John, Rose, William C., “Aerodynamic Effects” in The Infrared and Electro- Optical Systems Handbook, v. 2, Frederick G. Smith, Ed., SPIE Optical Engineering Press, 1993.

IR Handbook Seeing Analysis (cont.) Layer thickness (mks units): L: upstream heated length (m)  T: average temperature difference over upstream length (˚C) V: wind speed (m/s) Buoyancy termHydrodynamic term Assume: If  T < 0 then buoyancy term does not contribute to layer thickness.

Shell Seeing, Diffraction- Limited Error Budget Blue contours: rms wavefront error (nm) Acceptable operating range, assuming no AO correction. AO correction will extend the “green” area. = 500 nm

Shell Seeing, Seeing-Limited Error Budget Blue contours: 50% encircled energy (arcsec) Acceptable operating range = 1600 nm

Shell Seeing, Coronal Error Budget Blue contours: 50% encircled energy (arcsec) Acceptable operating range = 1000 nm

Dome Seeing (Inside/Outside Air  T) Correlation by Racine (1991) Approximate error budget Approximate  T requirement Need lots of passive flushing! Ref: Racine, Rene, “Mirror, dome, and natural seeing at CFHT,” PASP, v. 103, p. 1020, 1991.

IR Handbook aerodynamic treatment Correlation of Racine (1991) IR Handbook aerodynamic treatment Good seeing from KE test Ref: Racine, Rene, “Mirror, dome, and natural seeing at CFHT,” PASP, v. 103, p. 1020, BBSO Dome Seeing Experiments

Bad seeing from KE test BBSO Dome Seeing Experiments

A Nighttime Comparison: Gemini Dome 1 Duct exhaust fan on, low-moderate wind (3 - 5 m/s)  T = -3 ˚C Acceptable seeing observed with shell subcooled by 3 ˚C.

Bottom Line Requirements Enclosure skin temperature needs to be subcooled by up to 3 ˚C Interior air temperature needs to be within 0.5 ˚C of ambient outside air Need large passive flowrate to flush interior

Skin Energy Balance We want to use this term to control the skin temperature [~0 W/m 2 ] [377 W/m 2 ] [374 W/m 2 ] [98 W/m 2 ] [~100 W/m 2 ] Quantities vary by location on dome and weather conditions

Skin Thermal Control System Concept Concept Features: 1.White oxide paint a.Large  b.Small  s 2.Chilled skin a.Air b.Liquid (EGW) 3.Insulation prevents interior from being chilled by skin coolant

Shutter: air cooled, optional water cooling on lower end h air ~ 8 W/m 2 -K h H2O ~ 100 W/m 2 -K Enclosure support wall: water cooled if present h H2O ~ 100 W/m 2 -K Oblique skin panels: air cooled, h ~ 5 W/m 2 -K Sun-facing skin panels: air or water cooled h air ~ 5 W/m 2 -K h H2O ~ 100 W/m 2 -K Option: use fins on skin underside to increase effective area Skin Thermal Control System Concept (cont.)

Skin Cooling System Flow Loop Insert diagram here

MuSES Modeling: Validation at Gemini North Validation

Skin Thermal Control System Performance MuSES snapshot at 1430LT, 30 April 2003, Mauna Kea Wind speed = 0.5 m/s Ambient air T e = 7 – 8 ˚C Air Cooling Only on Skin ESW Water Cooled Most of surface is acceptable Sun-facing areas are ~ 5 ˚C hotter than ambient Surfaces that see cold sky subcool

MuSES snapshot at 1430LT, 30 April 2003, Mauna Kea Wind speed = 0.5 m/s Ambient air T e = 7 – 8 ˚C Air & Water Cooling Nearly all of surface is acceptably cool Sun-facing areas cooled with water Surfaces that see cold sky subcool Skin Thermal Control System Performance (cont.)

Cooling Requirements Next steps: Fan and system curves Heat exchanger specs Chiller specs Time response of fluid volume At peak heat load, surface cooling requires: Air-cooled skin: 56 kW Water-cooled skin: 18 kW Lower shutter: 14 kW Air-cooled shutter: 18 kW Total for carousel: 106 kW Enclosure support wall: 104 kW Grand total: 210 kW (60 tons)

Flushing System Concept 42 vent gates 168 m 2 flow area, each side

Flushing System Performance

Active Interior Ventilation Gemini volume flowrate: 10 enclosure volumes/hour (150,000 m 3 /hr) This flowrate on the smaller hybrid gives V ~ 0.2 m/s average Directed flow can give V~0.5 – 1 m/s over much of structure Fans may be mounted remotely or on carousel

Active Ventilation Issues Fan blades heat air  seeing Require homogenizing screens, cooling coils downstream of fans May not be simple to mount all this on carousel  possible to mount remotely

Shell Seeing Performance Blue contours: rms wavefront error (nm) Red: average  T of skin, front skin, shutter, lower shutter, ESW Most of the dome surface will give acceptable seeing Back of shutter subcools. May need to add water cooling there as well.