SloshSAT Colorado Space Grant Consortium Space Symposium Sage Andorka Dan Welsh Zach Sears Maurice Woods III Motoaki Honda 17 April 2010 1.

Slides:



Advertisements
Similar presentations
Study of Sloshing Effects, In Cylindrical Tanks
Advertisements

Chapter 5 Distributed Force. All of the forces we have used up until now have been forces applied at a single point. Most forces are not applied at a.
Coasting Phase Propellant Management for Upper Stages Philipp Behruzi Hans Strauch Francesco de Rose.
EAGE Dubai 12/11/ Interpretation of hydrocarbon microtremors as pore fluid oscillations driven by ambient seismic noise Marcel.
Advanced Topics in Heat, Momentum and Mass Transfer Lecturer Payman Jalali, Docent Faculty of Technology Dept. Energy & Environmental Technology Lappeenranta.
This slide intentionally left blank. The Rayleigh Plateau Instability By Mike Cromer and Patrick C. Rowe.
Chapter 16 Wave Motion.
Fluid Dynamics.
Abby Wilbourn, Department of Mechanical Engineering, CSU, Wallops Flight Facility Presentation, June 18, 2010.
SloshSAT Preliminary Design Review Dr. Robert Walch Dan Welsh Maurice Woods III Motoaki Honda Zach Sears 6/11/2010.
Preliminary Design Review Northwest Nazarene University Advisor: Dr. Lawrence Chad Larson Ben Gordon Seth Leija David Vinson Zach Thomas Drew Johnson.
Launch Readiness Review SloshSAT University of Northern Colorado Sage Andorka Dan Welsh Maurice Woods III Motoaki Honda Zach Sears 6/11/2010.
Linear Momentum and Collisions
An Introduction to Stress and Strain
Modeling Fluid Phenomena -Vinay Bondhugula (25 th & 27 th April 2006)
SloshSAT Conceptual Design Review Dr. Robert Walch Sage Andorka Dan Welsh Zach Sears Maurice Woods III Motoaki Honda Ryan Estrick 14 Oct
RockSat-C 2011 CoDR CSU RocketSat-C Conceptual Design Review Colorado State University Isaiah Franka Jordan Rath Abby Wilbourn Mike Yeager 10/1/10 1.
Numerical Hydraulics Wolfgang Kinzelbach with Marc Wolf and Cornel Beffa Lecture 1: The equations.
Module 3 Fluid Flow. Lesson 20 CONTINUITY EQUATION DESCRIBE how the density of a fluid varies with temperature. DEFINE the term buoyancy. DESCRIBE the.
(PDR ) University of Northern Colorado Nathan and Casey 11/14/08.
© 2011 Autodesk Freely licensed for use by educational institutions. Reuse and changes require a note indicating that content has been modified from the.
ME 231 Thermofluid Mechanics I Navier-Stokes Equations.
Waves - I Chapter 16 Copyright © 2014 John Wiley & Sons, Inc. All rights reserved.
1 Samara State Aerospace University (SSAU) Modern methods of analysis of the dynamics and motion control of space tether systems Practical lessons Yuryi.
Engineering Mechanics: Statics
Force on Floating bodies:
Formulation of a complete structural uncertainty model for robust flutter prediction Brian Danowsky Staff Engineer, Research Systems Technology, Inc.,
Four Forces of Flight Rocket Project Day 1. Aerodynamic Forces Act on a rocket as it flies through the air Lift & Drag Lift Force – Acts perpendicular.
CP502 Advanced Fluid Mechanics
Smoothed Particle Hydrodynamics (SPH) Fluid dynamics The fluid is represented by a particle system Some particle properties are determined by taking an.
Bernoulli’s Principle. Usually, liquids are considered “incompressible”, meaning that the density of the liquid remains nearly constant. Gases are easily.
Coupling Heterogeneous Models with Non-matching Meshes by Localized Lagrange Multipliers Modeling for Matching Meshes with Existing Staggered Methods and.
 In this section we will show the gruesome details in the derivation of the speed of sound in liquids:  In a taut string, potential energy is associated.
Performance Evaluation of Several Interpolation Methods for GPS Satellite Orbit Presented by Hamad Yousif Supervised by Dr. Ahmed El-Rabbany.
1 (a)Discrete Dynamical Systems : 1.Inverted Double Pendulum: Consider the double pendulum shown: 2.Some analytical models of nonlinear physical systems.
Computational fluid dynamics Authors: A. Ghavrish, Ass. Prof. of NMU, M. Packer, President of LDI inc.
Boyce/DiPrima 9 th ed, Ch 10.8 Appendix B: Derivation of the Wave Equation Elementary Differential Equations and Boundary Value Problems, 9 th edition,
MA402 Mathematics for Mechanical Engineering
Full Mission Simulation Test Report SloshSAT University of Northern Colorado Team Members: Sage Andorka Dan Welsh Motoaki Honda Maurice Woods III Zach.
USSC3002 Oscillations and Waves Lecture 1 One Dimensional Systems Wayne M. Lawton Department of Mathematics National University of Singapore 2 Science.
Waves - I Chapter 16 Copyright © 2014 John Wiley & Sons, Inc. All rights reserved.
Lecture 21-22: Sound Waves in Fluids Sound in ideal fluid Sound in real fluid. Attenuation of the sound waves 1.
Discretization Methods Chapter 2. Training Manual May 15, 2001 Inventory # Discretization Methods Topics Equations and The Goal Brief overview.
Chapter 11 Vibrations and Waves.
Monatomic Crystals.
By Anuraag Polisetty COSMOS Cluster 3
1 Linear Wave Equation The maximum values of the transverse speed and transverse acceleration are v y, max =  A a y, max =  2 A The transverse speed.
1.What are fluid kinematics?  kinematic descriptions of motion describe position, velocity, and accelerations (NOT FORCE) [ physical interpretation: what.
Authored by : Dr. Harold Alden Williams Montgomery College at the Takoma Park/Silver Spring Campus, Planetarium Director and Physics and Geology Laboratory.
EE Audio Signals and Systems Wave Basics Kevin D. Donohue Electrical and Computer Engineering University of Kentucky.
CSE 872 Dr. Charles B. Owen Advanced Computer Graphics1 Water Computational Fluid Dynamics Volumes Lagrangian vs. Eulerian modelling Navier-Stokes equations.
Scalar and Vector Quantities
Physics Topics 1. Motion 2. Measuring Matter 3. Work, Power, Machines 4. Newton’s Laws 5. Waves 6. Momentum 7. Pressure.
Sophomore Engineering Clinic I September 25, 2014 Blackboard Back of Room Section 12- Miller Section 13- Reed Section 13- Reed 1 Section 9- Tole Section.
Forces of Flight Flight and Space © 2011 Project Lead The Way, Inc.
Energy Reduction Through Tribology-2
Chapter 4 Fluid Mechanics Frank White
Figure 1. Spring characteristics
Figure 1. Spring characteristics
Forces of Flight Four Forces of Flight Gateway To Technology
Rocket Components and Design
Rocket Components and Design
Forces of Flight.
Forces of Flight Flight and Space © 2011 Project Lead The Way, Inc.
Optimized Vibration Mitigation in Design of Satellite Payload Support
Topic 6 NavierStokes Equations
Figure 1. Spring characteristics
Topic 8 Pressure Correction
APPLICATION OF LINEAR ALGEBRA IN MECHANICAL ENGINEERING
W L CG Dynamics Moment of Inertia LabRat Scientific © 2018.
Presentation transcript:

SloshSAT Colorado Space Grant Consortium Space Symposium Sage Andorka Dan Welsh Zach Sears Maurice Woods III Motoaki Honda 17 April

Liquid Slosh Forces produced by liquid fuel slosh can cause dramatic wobble during flight leading to control issues which may lead to failure of the mission. Years of research into fuel slosh has yielded computationally intensive models. This research begins with a simplified mathematical model which predicts the velocity profile of the fluid along a single axis. This model will be tested with an apparatus placed on the central axis of a two-stage Improved Terrier- Orion Sounding Rocket to be launched in June of If our experiment is successful, it may be possible in the future to generate a more comprehensive model. 2

Current Solutions Passive Attenuation A modeling system that accounts for both the motion of the spacecraft and the liquid fuel simultaneously is most ideal. This is very difficult as one can not control or measure the position or orientation of the fuel aboard the spacecraft accurately. It is only possible to measure the effects of the fuel slosh on the total system. As a result, many passive ways have been developed to dissipate the energy of the fuel sloshing:  Baffles,  Slosh absorbers,  Breaking a large tank into a smaller one However, these methods add weight and therefore increase launch costs. Traditional Modeling Methods Numerous analytical models have been used to describe the motion of fluids. The most accurate description of liquid motions requires use of the Navier-Stokes equations. These formulas, however, are not practical for control implementations as they are highly dependent on boundary conditions and are computationally intensive. Additional models have been suggested including  (Single and multi) mass-spring-damper  Pendulum liquid slug,  CFD/FEA models. (explain) 3

Our mathematical model will predict the movement of the fluid along the central axis. The spin of the rocket will produce a net force which will tend toward zero in the x- and y- plane. 4 To build the most general model, we look at the acceleration of a small volume element of the fluid: Mathematical Model Our project focuses on forces and our payload will collect acceleration data.

Mathematical Model 5 From the equations, we have too many variables to solve. The additional equations are continuity equations derived from conservation of mass considerations as well as an equation that relates a small change in a fluid element’s density to the resulting change in the pressure on that element through the bulk modulus.

Mathematical Model 6 Combining these equations gives the final expression for the fluid motion in the form of a wave equation in the z-direction: The solutions to this equation for which time and space separable (which does not include any driving forces): This equation represents the velocity profile of the fluid which takes the form of bi- directional traveling waves within the liquid. Boundary conditions and driving forces are needed to complete the model.

Expected Results If the canister and fluid behave as expected, the data we collect will yield a solution to the equation shown on the previous slide. Comparison of the data from the canisters movement with a control output will reveal if the system behaves in the manner that the model predicts. 7

Experiment Description A cylinder partially filled with Galden © will be constrained by an outer container so that it may only move along the central axis throughout the duration of the flight. The reason that we are using Galden © is for safety. The acceleration of the liquid cylinder will be recorded and these data will be combined with NASA rocket acceleration data and analyzed on the ground. The data collection electronics are the same as those designed by NASA for the Wallops RockOn! Workshop attended by UNC students in 2008.

Requirements Matrix RequirementMethodStatus The payload shall not weigh more than 3 kg.Design The payload shall not be more than tall 4.75”.Design The payload center of gravity (CG) shall be within 1” 3 of the geometric center. Design, Analysis The payload shall follow the no-volt requirement.Design The payload shall be self contained.Design The liquid shall not escape the redundant containment system. Design, Test The liquid shall not be conductive, corrosive, or flammable.Design, Test

Conclusions The project is scheduled to launch on June 24, 2010 from Wallops Flight Facility.

Thank You Solvey Solexis for the donation of Galden Jake Meyer at Avalis Wayfinding Solutions Inc for his machining Virginia and Colorado Space Grant Consortia for developing this program CSU for their support Dr. Robert Walch, Dr. Semak, and Dr. Gallovich for thier advising

References Clayburn, N., “Analytical Model of Liquid Slosh-Verification Experiment (SPLASHSAT)”, UNC Research Day, El-Sayad, M., Hanna, S., and Ibrahim, R., “Parametric Excitation of Nonlinear Elastic Systems involving Hydrodynamic Sloshing Impact,” Nonlinear Dynamics, Vol 18, 1999, pp Vreeburg, J.P.B., “Diagnosis of Water Motion in the Sloshsat FLEVO Tank”, National Aerospace Laboratory NLR, Walchko, K., “Robust Nonlinear Attitude Control with Disturbance Compensation”, Graduate Thesis, University of Florida, Anderson J., Turan, O., and Semercigil, S., “A Standing-wave Type Sloshing Absorber to Control Transient Oscillations,” Journal of Sound Vibration, Vol 232, No 5, 2000, pp Sidi, M., Spacecraft Dynamics and Controls, Cambridge University Press, New York, Hughes. P., Spacecraft Attitude Dynamics, John Wiley & Sons, New York, 1986.