Design of Unidirectional Freeze-Casting Device Members: John Simmonds Joe Hastings Michael Harty Michael Beachy Michael Cook (MET Department) Department.

Slides:



Advertisements
Similar presentations
Boiling heat transfer of liquid nitrogen in the presence of electric fields P Wang, P L Lewin, D J Swaffield and G Chen University of Southampton, Southampton,
Advertisements

Conduction Conceptests
Convection Temperature Device
Heat Transfer/Heat Exchanger
E(15-1) How is thermal energy transferred?
ME101-Basic Mechanical Engineering (STATICS) FRICTION
CASTING TECHNIQUES FOR SINGLE CRYSTAL GROWING (S.C.G.)
Density Is a physical property of matter
Heat Conduction of Zinc Specimen Femlab Simulation Measurement Calibration Technique: Effects of Heat Loss Through Specimen Surface Area.
UNIT 13 : HEAT 13.1 Thermal Conductivity 13.2 Thermal Expansion.
Inside-, Depth-, and Height-Measuring Instruments
Interim Design Amy Eckerle Andrew Whittington Philip Witherspoon Team 16.
Chapter 2: Overall Heat Transfer Coefficient
1 Attic thermal insulation The main issue in attic, superstructures in old districts and restoration works of roofs, is to create as much useful area as.
Applications Team Sensing Products
Measure the thermal conductivity Measure the thermal conductivity of silicon off-set with the stable state law School of Electronics & Applied Physics,
Team Members: Bryan McCormick (ME) Andy Freedman (ME) John Kreuder (ME) Ken McLoud (ME) Jon Holdsworth (EE) Gabriela Santa Cruz (IE) Thermoelectric Module.
Aim: What is density? Density: The concentration of matter in an object. Density is very IMPORTANT in the field of Earth Science. Why? Example: global.
Food Freezing Basic Concepts (cont'd) - Prof. Vinod Jindal
Thermopile Test Bench Team Thermopilers Adrian Aspinall, Paul Sowinski, David Eld, Michael Sotolongo,Tyler Merritt 1.
General idea of a couple of check rod system and adjustments
Kern Method of SHELL-AND-TUBE HEAT EXCHANGER Analysis
Measurements in Fluid Mechanics 058:180:001 (ME:5180:0001) Time & Location: 2:30P - 3:20P MWF 218 MLH Office Hours: 4:00P – 5:00P MWF 223B-5 HL Instructor:
DELTA Quadrant Tuning Y. Levashov, E. Reese. 2 Tolerances for prototype quadrant tuning Magnet center deviations from a nominal center line < ± 50  m.
Heat Transfer: Physical Origins and Rate Equations
S Temple CLRC1 End-cap Mechanics FDR Cooling Structures Steve Temple, RAL 1 November 2001.
M. D. A NDERSON Cancer Center Magnetic Resonance Imaging: 4.7 T, 40 cm Bruker Biospec James A Bankson, Ph.D. and John D Hazle, Ph.D. Small Animal Cancer.
LINEAR MEASUREMENT.
Installation. Indoor Unit Installation Typical Installation.
Two-Phase Heat Transfer Lab May 28-30, Analytical And Experimental Investigation of Evaporation from Porous Capillary Structures Presented to ONR.
1 Denis Grondin / Julien Giraud – 01 December 2008 SLAB COOLING Denis Grondin Julien Giraud
Measurements and Errors. Task: Find a textbook And measure it It doesn’t matter which textbook. It should have a length, a width and a height. Use the.
HP Automatic Liquid Handling (ALH)Hand Pipetted Method Takes 20 minutes per assayTakes 3 hours by a skilled worker 16 pL accuracy1 µl accuracy (1,000,000.
Development, Characterization, and Optimization of a Thermoelectric Generator System Lindsey Bunte, Jonny Hoskins, Tori Johnson, Shane McCauley School.
Design & Layout of Foodservice Facilities Reading Architectural Drawings Using the Architects’ Scale.
Energy transfer insulation Energy can be transferred from one location to another, as in the sun's energy travels through space to Earth. The two ways.
Chapter 2 Heat and Temperature. Heat & Temperature HEATTEMPERATURE DefinitionFlow of thermal energy Average kinetic energy Measuring DeviceCalorimeterThermometer.
Heat and Temperature Accuracy and Precision. Heat & Temperature HEATTEMPERATURE Definition Measuring Device Units.
Experimental and numerical studies on the bonfire test of high- pressure hydrogen storage vessels Prof. Jinyang Zheng Institute of Process Equipment, Zhejiang.
Rich Dewar Product Line Manager Itron. 2 THE DATTUS III METER / ’s1950’s1930’s1900’s DATTUS III.
Thermoelectric Cooling Team Members: Mark Campbell Peter Giles Andrew Smith Tom Strapps Nickolay Suther Team Supervisor: Dr. Prabir Basu Client: Greenfield.
SEPTEMBER 2002 Pixel Support Tube A. Smith LBNL 1 ATLAS Pixel Detector Heater Panel Testing Alexis Smith September 17, 2002.
Aircraft Carrier Draft Measurement Ship Draft Team - Fall 2015.
Introduction to Drafting and Design
Unidirectional Freeze Casting Group Status Report.
Measuring Instruments
Senior Design Team John Simmonds Joe Hastings Michael Harty
The Rayleigh-Taylor Instability By: Paul Canepa and Mike Cromer Team Leftovers.
Walter Sondheim 6/9/20081 DOE – Review of VTX upgrade detector for PHENIX Mechanics: Walter Sondheim - LANL.
Heat Transfer: Physical Origins and Rate Equations Chapter One Sections 1.1 and 1.2.
AIDA 1 Mezzanine board Resistors and capacitors near the ASiCs have now been relocated to the underside of the PCB. Cooling pads have been extended.
Heat Transfer Su Yongkang School of Mechanical Engineering # 1 HEAT TRANSFER CHAPTER 7 External flow.
Rapid Change Technology The following is a presentation to aid Technicians in the replacement of the Rapid Change Technology Block.
Heat transfer mechanism Dhivagar R Lecture 1 1. MECHANISMS OF HEAT TRANSFER Heat can be transferred in three different ways: conduction, convection, and.
Date of download: 9/17/2016 Copyright © ASME. All rights reserved. From: A Stepped-Bar Apparatus for Thermal Resistance Measurements J. Electron. Packag.
Turbo Installation Manipulator Final Design Review
Nano-fluidic Characterization
Heat and Temperature Accuracy and Precision.
Design of Unidirectional Freeze-Casting Device
Date of download: 10/14/2017 Copyright © ASME. All rights reserved.
Conduction.
Date of download: 10/23/2017 Copyright © ASME. All rights reserved.
Piyush Modi Assist.Prof
Chemical Engineering Explained
Date of download: 1/1/2018 Copyright © ASME. All rights reserved.
Chapter 8 : Natural Convection
Date of download: 3/4/2018 Copyright © ASME. All rights reserved.
Conditions and procedures of Japan research
ICHS5 – 2013 September, Brussels, Belgium | ID161
Forced Convection Trials at 100°C Natural Convection Trials at 100°C
Presentation transcript:

Design of Unidirectional Freeze-Casting Device Members: John Simmonds Joe Hastings Michael Harty Michael Beachy Michael Cook (MET Department) Department of Mechanical and Aerospace Engineering Old Dominion University, Norfolk, VA 23529

Gantt Chart

Actual Freeze-casting device Freeze-casting device Schematic Equipment Design

Proposed Changes to Freezing Device Both arms on one supporting rod enables direct measurement transference between them. Current Freezing Device Two separate arms. One for liquid height measurement and one for sample height Proposed Liquid Level indicator arm Sample Arm Dewar Liquid Nitrogen Height Adjustment Nut

Thermal Measuring System K type thermocouples do not have a high enough degree of accuracy for our experimental system. (Standard: +/- 2.2C or +/-.75%) Due to this issue, a different thermal measuring system was installed to more accurately and precisely detect the temperature gradients during ceramic slurry trials. T type thermocouples replaced the K Types and new data logging software and interface have been installed.

Thermocouple The T type thermocouple is the current sensor used to understand freeze front velocities within our experiment. We replaced the K type thermocouple along with the data acquisition interface for the T type thermocouple and the Omega QuadTemp interface. The improvements are seen by a greater degree of accuracy within the temperature range of our experiment. Another improvement with the new interface can be seem with the ability to use four thermocouples vice the two that were supported by the Vernier Data Logger.

Convective Boundary Layer Omission The insulating sleeve, as previously discussed reduced the convective effects of the surrounding nitrogen gas on the sides of the sample. This allowed the sample to be frozen from the bottom upwards only. The original sleeve was made from a high density polyethylene foam and although fit snuggly it allowed a small convective current around the plate. The new sleeve is made from a low density Styrofoam. The sleeve is made from (4) individual sections that were glued together, wherein the lowest section center chamber was made to a smaller diameter that allows the plate to rest on and blocks the convective layers. Present Freeze-casting device Configuration

Convective Boundary Layer Omission The new sleeve is made from a low density Styrofoam. The sleeve is made from (4) individual sections that were glued together, wherein the lowest section center chamber was made to a smaller diameter that allows the plate to rest on and blocks the convective layers. Dewar insulating Sleeve

Sample Analysis Currently, samples have been produced at the following heights above liquid level: 20mm, 25mm, 30mm, 35mm, 40mm, 45mm, 50mm, 55mm, 60mm and 65mm. The samples were freeze-dried and begun to be sintered. The initial inspection under a 10x and 100x microscope show promising signs of unidirectional platelet formation and alignment.