Quasi Steady Air Loads Report: Flat Plate With Central Load

Size: px
Start display at page:

Download "Quasi Steady Air Loads Report: Flat Plate With Central Load"

Transcription

1 Quasi Steady Air Loads Report: Flat Plate With Central Load Sorin Pirau, Alexander Forbes, Brandon Liberi, Vrishank Raghav, Narayanan Komerath Experimental Aerodynamics and Concepts Group Daniel Guggenheim School of Aerospace Engineering Georgia Institute of Technology Atlanta, Georgia USA Contact: February 24, 2015

2 Report Number ADLP February 24,

3 Summary The variation of quasi-steady air loads with attitude on a flat plate model with a cylindrical load centered on its upper surface, is described. The loads are ensemble-averaged with 1-degree resolution using the Continuous Rotation technique, with a stepper motor rotating at 0.99 RPM above a 6- DOF load cell. The azimuthal variation is reduced to a Fourier series. A truncated series of Fourier coefficients is listed. This is seen to represent the load variations with adequate accuracy for use in dynamic simulation. Cases included those at zero pitch and at -10 degrees pitch. 2

4 Contents 1 Description 4 2 Model Geometry 5 3 Results-Fourier Coefficients m/s (20 Mph), Flat Edge facing the flow, Pitch -10 deg m/s (20 Mph), Sharp Edge facing the flow, Pitch -10 deg m/s (30 Mph), Flat Edge facing the flow, Pitch -10 deg m/s (30 Mph), Sharp Edge facing the flow, Pitch -10 deg

5 Chapter 1 Description The Flat plate is composed of plexi-glass, with an aluminum cylinder placed on top, which connects the flat plate to a thin cylindrical rod of length m (10.5in) and diameter of m (3/8 in). The aluminum cylinder ensures that the metal rod is flush to the surface of the flat plate and there are no gaps between the rod and the flat plate to interact with the flow. It is to be noted that the metal rod goes through the flat plate and into the aluminum cylinder, and thus only m (8.625in) of the metal rod is exposed to the airflow. The cylindrical rod is used as a mounting strut for the model. A continuous rotation method is used in order to obtain load data about the flat plate for incrimental changes in yaw. The model is rotated at an RPM of 0.99 for 10 revolutions, after which the data obtained is phase averaged and ensemble averaged to a resolution of 1 degree. After the data is averaged, Fast Fourier Transform can be used on the data to estimate the coefficients of a trigonometric polynomial that interpolates each individual set of data, Cx, Cy, Cz, CMx, CMy, CMz. Only the first 20 coefficients are used, thus during simulations, it is more efficient to interpolate/calculate the load values from the Fourier coefficients than by looking up and extracting the required values from a data set. This paper lists the coefficients for these Fourier series representations so that they may be used instead of the actual data points. In order to interpolate the data, a trigonometric polynomial of the form shown in Equation 1.1 was used. y = a 0 + b 0 + a 1 cos(2π(x/360)) + b 1 sin(2π(x/360) + a 2 cos(2π(2x/360)) + b 2 sin(2π(2x/360) a 2 0cos(2π(20x/360)) + b 2 0sin(2π(20x/360) (1.1) The conditions for which the flat plate was tested are listed before each data set and the geometric dimensions of the flat plate are listed in Chapter 2 of this report. The flat plate was tested for two configurations at two different velocities/reynolds numbers. It was found through close examination of the flat plate, that one of the long sides of the flat plate had a flat edge where it was cut and the other side had a sharp/angled edge. Therefore the flat plate was tested at a -10 deg initial pitch, first with the flat edge facing the flow, and second with the sharp edge facing the flow. Figure 1.1: Flatplate model 4

6 Chapter 2 Model Geometry Table 2.1: Experimental Velocities Tested Experimental Velocities Tested Velocity (mph) Velocity (m/s) Table 2.2: Model Geometry Model Geometry Flat Plate Length (m) Flat Plate Width (m) Flat Plate Height (m) Area Used for Coefficients (m 2 ) Moment Arm Used for Coefficients (m)

7 Chapter 3 Results-Fourier Coefficients m/s (20 Mph), Flat Edge facing the flow, Pitch -10 deg Table 3.1: Experimental Conditions Experimental Conditions Tempterature (F) 74.2 Pressure (inhg) Density Calculated (kg/m 3 ) Density Used (kg/m 3 ) Table 3.2: A-Fourier Coefficients A-Fourier Coefficients Number CD CY CZ CMX CMY CMZ E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E-06 6

8 Table 3.3: B-Fourier Coefficients B-Fourier Coefficients Number CD CY CZ CMX CMY CMZ E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E-06 7

9 8

10 9

11 10

12 m/s (20 Mph), Sharp Edge facing the flow, Pitch -10 deg Table 3.4: Experimental Conditions Experimental Conditions Tempterature (F) 74.2 Pressure (inhg) Density Calculated (kg/m 3 ) Density Used (kg/m 3 ) Table 3.5: A-Fourier Coefficients A-Fourier Coefficients Number CD CY CZ CMX CMY CMZ E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E-06 11

13 Table 3.6: B-Fourier Coefficients B-Fourier Coefficients Number CD CY CZ CMX CMY CMZ E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E-05 12

14 13

15 14

16 15

17 m/s (30 Mph), Flat Edge facing the flow, Pitch -10 deg Table 3.7: Experimental Conditions Experimental Conditions Tempterature (F) 74.2 Pressure (inhg) Density Calculated (kg/m 3 ) Density Used (kg/m 3 ) Table 3.8: A-Fourier Coefficients A-Fourier Coefficients Number CD CY CZ CMX CMY CMZ E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E-06 16

18 Table 3.9: B-Fourier Coefficients B-Fourier Coefficients Number CD CY CZ CMX CMY CMZ E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E-05 17

19 18

20 19

21 20

22 m/s (30 Mph), Sharp Edge facing the flow, Pitch -10 deg Table 3.10: Experimental Conditions Experimental Conditions Tempterature (F) 74.2 Pressure (inhg) Density Calculated (kg/m 3 ) Density Used (kg/m 3 ) Table 3.11: A-Fourier Coefficients A-Fourier Coefficients Number CD CY CZ CMX CMY CMZ E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E-06 21

23 Table 3.12: B-Fourier Coefficients B-Fourier Coefficients Number CD CY CZ CMX CMY CMZ E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E-05 22

24 23

25 24

26 25

Quasi Steady Air Loads Report: CUBOID

Quasi Steady Air Loads Report: CUBOID Quasi Steady Air Loads Report: CUBOID Sorin Pirau, Alexander Forbes, Brandon Liberi, Vrishank Raghav, Narayanan Komerath Experimental Aerodynamics and Concepts Group Daniel Guggenheim School of Aerospace

More information

Efficient Modeling of Dynamic Blockage Effects for Unsteady Wind Tunnel Testing

Efficient Modeling of Dynamic Blockage Effects for Unsteady Wind Tunnel Testing Efficient Modeling of Dynamic Blockage Effects for Unsteady Wind Tunnel Testing Sumant Sharma ssharma46@gatech.edu Undergraduate Research Assistant Narayanan Komerath komerath@gatech.edu Professor Vrishank

More information

Exploration of the Physics of Hub Drag

Exploration of the Physics of Hub Drag Exploration of the Physics of Hub Drag Felipe Ortega, Rajiv Shenoy, Vrishank Raghav Marilyn Smith and Narayanan Komerath Daniel Guggenheim Georgia Institute of Technology AIAA ASM Conference, Nashville

More information

Deconstructing Hub Drag: Final Report on Experiments

Deconstructing Hub Drag: Final Report on Experiments DISTRIBUTION STATEMENT A: Distribution approved for public release; distribution is unlimited. Deconstructing Hub Drag: Final Report on Experiments Alexander H. Forbes, Vrishank S. Raghav, Michael Mayo,

More information

PLUME MODELING AND APPLICATION TO MARS 2001 ODYSSEY AEROBRAKING

PLUME MODELING AND APPLICATION TO MARS 2001 ODYSSEY AEROBRAKING PLUME MODELING AND APPLICATION TO MARS ODYSSEY AEROBRAKING Zachary Q. Chavis Joint Institute for Advancement of Flight Sciences The George Washington University NASA Langley Research Center Hampton, VA

More information

Numerical analysis of the influence of particular autogyro parts on the aerodynamic forces

Numerical analysis of the influence of particular autogyro parts on the aerodynamic forces Numerical analysis of the influence of particular autogyro parts on the aerodynamic forces Zbigniew Czyż 1,*, Paweł Karpiński 1, Tomasz Łusiak 2, and Tomasz Szczepanik 3 1 Lublin University of Technology,

More information

Massachusetts Institute of Technology Department of Electrical Engineering and Computer Science Electric Machines

Massachusetts Institute of Technology Department of Electrical Engineering and Computer Science Electric Machines Massachusetts Institute of Technology Department of Electrical Engineering and Computer Science 6.685 Electric Machines Problem Set 10 Issued November 11, 2013 Due November 20, 2013 Problem 1: Permanent

More information

Selection Calculations For Linear & Rotary Actuators

Selection Calculations For Linear & Rotary Actuators H-8 For Electric Linear Slides and Electric Cylinders First determine your series, then select your product. Select the actuator that you will use based on the following flow charts: Selection Procedure

More information

A Balance for Measurement of Yaw, Lift and Drag on a Model in a Hypersonic Shock Tunnel

A Balance for Measurement of Yaw, Lift and Drag on a Model in a Hypersonic Shock Tunnel , July 6-8, 2011, London, U.K. A Balance for Measurement of Yaw, Lift and Drag on a Model in a Hypersonic Shock Tunnel S. Trivedi, and V. Menezes Abstract This paper describes the design of an accelerometer

More information

Fan Stage Broadband Noise Benchmarking Programme

Fan Stage Broadband Noise Benchmarking Programme Fan Stage Broadband Noise Benchmarking Programme Specification of Fundamental Test Case 3 (FC3) Version 1 : 26 January 2015 Test Case Coordinator John Coupland ISVR University of Southampton UK E-mail

More information

Experiment Design to Obtain Unsteady Force and Moment Data on a Yawing Submarine Model - Sept. 2011

Experiment Design to Obtain Unsteady Force and Moment Data on a Yawing Submarine Model - Sept. 2011 Experiment Design to Obtain Unsteady Force and Moment Data on a Yawing Submarine Model - Sept. 2011 Problem: This problem is to determine (1) the desired values of fixed parameters and (2) the required

More information

TutorBreeze.com 7. ROTATIONAL MOTION. 3. If the angular velocity of a spinning body points out of the page, then describe how is the body spinning?

TutorBreeze.com 7. ROTATIONAL MOTION. 3. If the angular velocity of a spinning body points out of the page, then describe how is the body spinning? 1. rpm is about rad/s. 7. ROTATIONAL MOTION 2. A wheel rotates with constant angular acceleration of π rad/s 2. During the time interval from t 1 to t 2, its angular displacement is π rad. At time t 2

More information

Wings and Bodies in Compressible Flows

Wings and Bodies in Compressible Flows Wings and Bodies in Compressible Flows Prandtl-Glauert-Goethert Transformation Potential equation: 1 If we choose and Laplace eqn. The transformation has stretched the x co-ordinate by 2 Values of at corresponding

More information

ANALYSIS AND OPTIMIZATION OF A VERTICAL AXIS WIND TURBINE SAVONIUS-TYPE PANEL USING CFD TECHNIQUES

ANALYSIS AND OPTIMIZATION OF A VERTICAL AXIS WIND TURBINE SAVONIUS-TYPE PANEL USING CFD TECHNIQUES ANALYSIS AND OPTIMIZATION OF A VERTICAL AXIS WIND TURBINE SAVONIUS-TYPE PANEL USING CFD TECHNIQUES J. Vilarroig, S. Chiva*, R. Martínez and J. Segarra** *Author for correspondence ** Heliotec.SL Department

More information

Mestrado Integrado em Engenharia Mecânica Aerodynamics 1 st Semester 2012/13

Mestrado Integrado em Engenharia Mecânica Aerodynamics 1 st Semester 2012/13 Mestrado Integrado em Engenharia Mecânica Aerodynamics 1 st Semester 212/13 Exam 2ª época, 2 February 213 Name : Time : 8: Number: Duration : 3 hours 1 st Part : No textbooks/notes allowed 2 nd Part :

More information

AP Physics C. Gauss s Law. Free Response Problems

AP Physics C. Gauss s Law. Free Response Problems AP Physics Gauss s Law Free Response Problems 1. A flat sheet of glass of area 0.4 m 2 is placed in a uniform electric field E = 500 N/. The normal line to the sheet makes an angle θ = 60 ẘith the electric

More information

CHAPTER 8: ROTATIONAL OF RIGID BODY PHYSICS. 1. Define Torque

CHAPTER 8: ROTATIONAL OF RIGID BODY PHYSICS. 1. Define Torque 7 1. Define Torque 2. State the conditions for equilibrium of rigid body (Hint: 2 conditions) 3. Define angular displacement 4. Define average angular velocity 5. Define instantaneous angular velocity

More information

A Comparison of Force Balance and Pressure Integration Techniques for Predicting Wind-Induced Responses of Tall Buildings

A Comparison of Force Balance and Pressure Integration Techniques for Predicting Wind-Induced Responses of Tall Buildings A Comparison of Force Balance and Pressure Integration Techniques for Predicting Wind-Induced Responses of Tall Buildings Authors: Calin Dragoiescu, Jason Garber and K. Suresh Kumar RWDI, 650 Woodlawn

More information

Exam 3--Fall 08--PHYS 101

Exam 3--Fall 08--PHYS 101 Name: Class: Date: Exam 3--Fall 08--PHYS 101 Multiple Choice Identify the choice that best completes the statement or answers the question. 1. An object at rest begins to rotate with a constant angular

More information

EDUCATIONAL WIND TUNNEL

EDUCATIONAL WIND TUNNEL EDUCATIONAL WIND TUNNEL AEROLAB LLC 8291 Patuxent Range Road Suite 1200 Jessup, MD 20794 Phone: 301.776.6585 Fax: 301.776.2892 contact@aerolab.com www.aerolab.com EDUCATIONAL WIND TUNNEL Conceived in 1947

More information

Mechanics of Flight. Warren F. Phillips. John Wiley & Sons, Inc. Professor Mechanical and Aerospace Engineering Utah State University WILEY

Mechanics of Flight. Warren F. Phillips. John Wiley & Sons, Inc. Professor Mechanical and Aerospace Engineering Utah State University WILEY Mechanics of Flight Warren F. Phillips Professor Mechanical and Aerospace Engineering Utah State University WILEY John Wiley & Sons, Inc. CONTENTS Preface Acknowledgments xi xiii 1. Overview of Aerodynamics

More information

Experimental Aerodynamics. Experimental Aerodynamics

Experimental Aerodynamics. Experimental Aerodynamics Lecture 3: Vortex shedding and buffeting G. Dimitriadis Buffeting! All structures exposed to a wind have the tendency to vibrate.! These vibrations are normally of small amplitude and have stochastic character!

More information

AE 3051, Lab #16. Investigation of the Ideal Gas State Equation. By: George P. Burdell. Group E3

AE 3051, Lab #16. Investigation of the Ideal Gas State Equation. By: George P. Burdell. Group E3 AE 3051, Lab #16 Investigation of the Ideal Gas State Equation By: George P. Burdell Group E3 Summer Semester 000 Abstract The validity of the ideal gas equation of state was experimentally tested for

More information

EMA 3702 Mechanics & Materials Science (Mechanics of Materials) Chapter 3 Torsion

EMA 3702 Mechanics & Materials Science (Mechanics of Materials) Chapter 3 Torsion EMA 3702 Mechanics & Materials Science (Mechanics of Materials) Chapter 3 Torsion Introduction Stress and strain in components subjected to torque T Circular Cross-section shape Material Shaft design Non-circular

More information

Code No: R Set No. 1

Code No: R Set No. 1 Code No: R05010302 Set No. 1 I B.Tech Supplimentary Examinations, February 2008 ENGINEERING MECHANICS ( Common to Mechanical Engineering, Mechatronics, Metallurgy & Material Technology, Production Engineering,

More information

Models of Lift and Drag Coefficients of Stalled and Unstalled Airfoils in Wind Turbines and Wind Tunnels

Models of Lift and Drag Coefficients of Stalled and Unstalled Airfoils in Wind Turbines and Wind Tunnels NASA/CR 2008-215434 Models of Lift and Drag Coefficients of Stalled and Unstalled Airfoils in Wind Turbines and Wind Tunnels David A. Spera Jacobs Technology, Inc., Cleveland, Ohio October 2008 NASA STI

More information

CH. 5 TRUSSES BASIC PRINCIPLES TRUSS ANALYSIS. Typical depth-to-span ratios range from 1:10 to 1:20. First: determine loads in various members

CH. 5 TRUSSES BASIC PRINCIPLES TRUSS ANALYSIS. Typical depth-to-span ratios range from 1:10 to 1:20. First: determine loads in various members CH. 5 TRUSSES BASIC PRINCIPLES Typical depth-to-span ratios range from 1:10 to 1:20 - Flat trusses require less overall depth than pitched trusses Spans: 40-200 Spacing: 10 to 40 on center - Residential

More information

Advanced Vibrations. Distributed-Parameter Systems: Exact Solutions (Lecture 10) By: H. Ahmadian

Advanced Vibrations. Distributed-Parameter Systems: Exact Solutions (Lecture 10) By: H. Ahmadian Advanced Vibrations Distributed-Parameter Systems: Exact Solutions (Lecture 10) By: H. Ahmadian ahmadian@iust.ac.ir Distributed-Parameter Systems: Exact Solutions Relation between Discrete and Distributed

More information

Magnetic Field Measurement System For Cryogenic Permanent Magnet Undulator At SSRF

Magnetic Field Measurement System For Cryogenic Permanent Magnet Undulator At SSRF Magnetic Field Measurement System For Cryogenic Permanent Magnet Undulator At SSRF Hongfei Wang, Jingmin Zhang,Wei Zhang, Qiaogen Zhou Shanghai Institute of Applied Physics, P.O.Box 800-204, Shanghai 201800,

More information

Case Studies for Uncertainty Quantification of a High-fidelity Spacecraft Oriented Break-up Tool. Bent Fritsche, HTG Stijn Lemmens, ESA

Case Studies for Uncertainty Quantification of a High-fidelity Spacecraft Oriented Break-up Tool. Bent Fritsche, HTG Stijn Lemmens, ESA Case Studies for Uncertainty Quantification of a High-fidelity Spacecraft Oriented Break-up Tool Bent Fritsche, HTG Stijn Lemmens, ESA 8th European Symposium on Aerothermodynamics for Space Vehicles Lisbon,

More information

SOLUTION 8 7. To hold lever: a+ M O = 0; F B (0.15) - 5 = 0; F B = N. Require = N N B = N 0.3. Lever,

SOLUTION 8 7. To hold lever: a+ M O = 0; F B (0.15) - 5 = 0; F B = N. Require = N N B = N 0.3. Lever, 8 3. If the coefficient of static friction at is m s = 0.4 and the collar at is smooth so it only exerts a horizontal force on the pipe, determine the minimum distance x so that the bracket can support

More information

Contents. Chapter 1 Introduction Chapter 2 Unacceptable Cam Curves Chapter 3 Double-Dwell Cam Curves... 27

Contents. Chapter 1 Introduction Chapter 2 Unacceptable Cam Curves Chapter 3 Double-Dwell Cam Curves... 27 Contents Chapter 1 Introduction... 1 1.0 Cam-Follower Systems... 1 1.1 Fundamentals... 1 1.2 Terminology... 4 Type of Follower Motion... 4 Type of Joint Closure... 4 Type of Follower... 5 Type of Cam...

More information

ADMISSION TEST INDUSTRIAL AUTOMATION ENGINEERING

ADMISSION TEST INDUSTRIAL AUTOMATION ENGINEERING UNIVERSITÀ DEGLI STUDI DI PAVIA ADMISSION TEST INDUSTRIAL AUTOMATION ENGINEERING September 26, 2016 The candidates are required to answer the following multiple choice test which includes 30 questions;

More information

Rotational Mechanics Part III Dynamics. Pre AP Physics

Rotational Mechanics Part III Dynamics. Pre AP Physics Rotational Mechanics Part III Dynamics Pre AP Physics We have so far discussed rotational kinematics the description of rotational motion in terms of angle, angular velocity and angular acceleration and

More information

Detumbling an Uncontrolled Satellite with Contactless Force by Using an Eddy Current Brake

Detumbling an Uncontrolled Satellite with Contactless Force by Using an Eddy Current Brake 213 IEEE/RSJ International Conference on Intelligent Robots and Systems (IROS) November 3-7, 213. Tokyo, Japan Detumbling an Uncontrolled Satellite with Contactless Force by Using an Eddy Current Brake

More information

NAL 60CM MAGNETIC SUSPENSION AND BALANCE SYSTEM

NAL 60CM MAGNETIC SUSPENSION AND BALANCE SYSTEM NAL 60CM MAGNETC SUSPENSON AND BALANCE SYSTEM Hideo Sawada Shinichi Suda Tetsuya Kunimasu JAXA the nstitute of Space Technology and Aeronautics (STA) Keywords: Wind tunnel tests balance support control

More information

Design and modelling of an airship station holding controller for low cost satellite operations

Design and modelling of an airship station holding controller for low cost satellite operations AIAA Guidance, Navigation, and Control Conference and Exhibit 15-18 August 25, San Francisco, California AIAA 25-62 Design and modelling of an airship station holding controller for low cost satellite

More information

Volumes of Solids of Revolution. We revolve this curve about the x-axis and create a solid of revolution.

Volumes of Solids of Revolution. We revolve this curve about the x-axis and create a solid of revolution. Volumes of Solids of Revolution Consider the function ( ) from a = to b = 9. 5 6 7 8 9 We revolve this curve about the x-axis and create a solid of revolution. - 5 6 7 8 9 - - - We want to find the volume

More information

DISTRIBUTED BY: National Technical iormatiuo Service U. S. DEPARTMENT OF COMMERCE AD BOUNDARY-LAYER STUDIES ON SPINNING BODIES OF REVOLUTION

DISTRIBUTED BY: National Technical iormatiuo Service U. S. DEPARTMENT OF COMMERCE AD BOUNDARY-LAYER STUDIES ON SPINNING BODIES OF REVOLUTION AD-785 688 BOUNDARY-LAYER STUDIES ON SPINNING BODIES OF REVOLUTION Walter B. Sturek Ballistic Research Laboratories Aberdeen Proving Ground, Maryland 1973 DISTRIBUTED BY: National Technical iormatiuo Service

More information

The principle of the flywheel is found before the many centuries ago in spindle and the potter's wheel.

The principle of the flywheel is found before the many centuries ago in spindle and the potter's wheel. TOM Fly Wheel Mechanical Engineering Department The principle of the flywheel is found before the many centuries ago in spindle and the potter's wheel. A heavy-rimmed rotating wheel used to minimize variations

More information

German Aerospace Center (DLR)

German Aerospace Center (DLR) German Aerospace Center (DLR) AEROGUST M30 Progress Meeting 23-24 November 2017, Bordeaux Presented by P. Bekemeryer / J. Nitzsche With contributions of C. Kaiser 1, S. Görtz 2, R. Heinrich 2, J. Nitzsche

More information

Mixing Process of Binary Polymer Particles in Different Type of Mixers

Mixing Process of Binary Polymer Particles in Different Type of Mixers Vol. 3, No. 6 Mixing Process of Binary Polymer Particles in Different Type of Mixers S.M.Tasirin, S.K.Kamarudin & A.M.A. Hweage Department of Chemical and Process Engineering, Universiti Kebangsaan Malaysia

More information

Fig. 6.1 Plate or disk cam.

Fig. 6.1 Plate or disk cam. CAMS INTRODUCTION A cam is a mechanical device used to transmit motion to a follower by direct contact. The driver is called the cam and the driven member is called the follower. In a cam follower pair,

More information

IDENTIFICATION OF SHIP PROPELLER TORSIONAL VIBRATIONS

IDENTIFICATION OF SHIP PROPELLER TORSIONAL VIBRATIONS Journal of KONES Powertrain and Transport, Vol., No. 015 IDENTIFICATION OF SHIP PROPELLER TORSIONAL VIBRATIONS Jan Rosłanowski Gdynia Maritime University, Faculty of Marine Engineering Morska Street 81-87,

More information

UNIT 4 FLYWHEEL 4.1 INTRODUCTION 4.2 DYNAMICALLY EQUIVALENT SYSTEM. Structure. Objectives. 4.1 Introduction

UNIT 4 FLYWHEEL 4.1 INTRODUCTION 4.2 DYNAMICALLY EQUIVALENT SYSTEM. Structure. Objectives. 4.1 Introduction UNIT 4 FLYWHEEL Structure 4.1 Introduction Objectives 4. Dynamically Equivalent System 4.3 Turning Moment Diagram 4.3.1 Turning Moment Diagram of a Single Cylinder 4-storke IC Engine 4.3. Turning Moment

More information

ScienceDirect. Optimization of the size and launch conditions of a discus

ScienceDirect. Optimization of the size and launch conditions of a discus Available online at www.sciencedirect.com ScienceDirect Procedia Engineering 72 ( 24 ) 756 76 The 24 conference of the International Sports Engineering Association Optimization of the size and launch conditions

More information

MA 114 Worksheet # 1: Improper Integrals

MA 114 Worksheet # 1: Improper Integrals MA 4 Worksheet # : Improper Integrals. For each of the following, determine if the integral is proper or improper. If it is improper, explain why. Do not evaluate any of the integrals. (c) 2 0 2 2 x x

More information

Wind Tunnel Study of a Large Aerostat, CFD Validation

Wind Tunnel Study of a Large Aerostat, CFD Validation AIAA Lighter-Than-Air Systems Technology (LTA) Conference 25-28 March 2013, Daytona Beach, Florida AIAA 2013-1339 Wind Tunnel Study of a Large Aerostat, CFD Validation Stephen C. Chan 1, Kaleb Shervington

More information

LINE TECH Linear Modules. Ready to built-in linear modules with drive

LINE TECH Linear Modules. Ready to built-in linear modules with drive Ready to built-in linear modules with drive Anodized profile, produced in extrusion molding method Linear rail guiding system (LM3 LM5) Actuation by ball screw, high-helix lead _ screw or toothed belt

More information

MATH Final Review

MATH Final Review MATH 1592 - Final Review 1 Chapter 7 1.1 Main Topics 1. Integration techniques: Fitting integrands to basic rules on page 485. Integration by parts, Theorem 7.1 on page 488. Guidelines for trigonometric

More information

QUESTION BANK SEMESTER: III SUBJECT NAME: MECHANICS OF SOLIDS

QUESTION BANK SEMESTER: III SUBJECT NAME: MECHANICS OF SOLIDS QUESTION BANK SEMESTER: III SUBJECT NAME: MECHANICS OF SOLIDS UNIT 1- STRESS AND STRAIN PART A (2 Marks) 1. Define longitudinal strain and lateral strain. 2. State Hooke s law. 3. Define modular ratio,

More information

General Definition of Torque, final. Lever Arm. General Definition of Torque 7/29/2010. Units of Chapter 10

General Definition of Torque, final. Lever Arm. General Definition of Torque 7/29/2010. Units of Chapter 10 Units of Chapter 10 Determining Moments of Inertia Rotational Kinetic Energy Rotational Plus Translational Motion; Rolling Why Does a Rolling Sphere Slow Down? General Definition of Torque, final Taking

More information

Three-Dimensional Features of the Stalled Flow field of a Rotor Blade in Forward Flight

Three-Dimensional Features of the Stalled Flow field of a Rotor Blade in Forward Flight Three-Dimensional Features of the Stalled Flow field of a Rotor Blade in Forward Flight Vrishank Raghav, Phillip Richards, Narayanan Komerath, Marilyn Smith Daniel Guggenheim School of Aerospace Engineering,

More information

Characterization of the wind loads and flow fields around a gable-roof building model in tornado-like winds

Characterization of the wind loads and flow fields around a gable-roof building model in tornado-like winds Exp Fluids (211) 51:835 851 DOI 1.17/s348-11-112-6 RESEARCH ARTICLE Characterization of the wind loads and flow fields around a gable-roof building model in tornado-like winds Hui Hu Zifeng Yang Partha

More information

Velocity measurements on a retreating blade in dynamic stall

Velocity measurements on a retreating blade in dynamic stall Experiments in Fluids manuscript No. (will be inserted by the editor) Velocity measurements on a retreating blade in dynamic stall Vrishank Raghav Narayanan Komerath Received: 5 September 2013/Revised:

More information

PRINCIPLES OF FLIGHT

PRINCIPLES OF FLIGHT 1 Considering a positive cambered aerofoil, the pitching moment when Cl=0 is: A infinite B positive (nose-up). C negative (nose-down). D equal to zero. 2 The angle between the aeroplane longitudinal axis

More information

A novel fluid-structure interaction model for lubricating gaps of piston machines

A novel fluid-structure interaction model for lubricating gaps of piston machines Fluid Structure Interaction V 13 A novel fluid-structure interaction model for lubricating gaps of piston machines M. Pelosi & M. Ivantysynova Department of Agricultural and Biological Engineering and

More information

SPC Aerodynamics Course Assignment Due Date Monday 28 May 2018 at 11:30

SPC Aerodynamics Course Assignment Due Date Monday 28 May 2018 at 11:30 SPC 307 - Aerodynamics Course Assignment Due Date Monday 28 May 2018 at 11:30 1. The maximum velocity at which an aircraft can cruise occurs when the thrust available with the engines operating with the

More information

Matlab Sheet 2. Arrays

Matlab Sheet 2. Arrays Matlab Sheet 2 Arrays 1. a. Create the vector x having 50 logarithmically spaced values starting at 10 and ending at 1000. b. Create the vector x having 20 logarithmically spaced values starting at 10

More information

0.5 rad r C 20 mm. 30 deg r s 50 mm. r A. 200 mm. Solution: v C 0.01 m s. v C. r s. 0.2 rad. v A v E s r A

0.5 rad r C 20 mm. 30 deg r s 50 mm. r A. 200 mm. Solution: v C 0.01 m s. v C. r s. 0.2 rad. v A v E s r A 16 29. The mechanim for a car window winder i hown in the figure. Here the handle turn the mall cog C, which rotate the pur gear S, thereby rotating the fixed-connected lever which raie track D in which

More information

ENAE 483: Principles of Space System Design Loads, Structures, and Mechanisms

ENAE 483: Principles of Space System Design Loads, Structures, and Mechanisms ENAE 483: Principles of Space System Design Loads, Structures, and Mechanisms Team: Vera Klimchenko Kevin Lee Kenneth Murphy Brendan Smyth October 29 th, 2012 Presentation Overview Project Overview Mission

More information

Reduced-order modelling and parameter estimation for a quarter-car suspension system

Reduced-order modelling and parameter estimation for a quarter-car suspension system 81 Reduced-order modelling and parameter estimation for a quarter-car suspension system C Kim and PIRo* Department of Mechanical and Aerospace Engineering, North Carolina State University, Raleigh, North

More information

Engineering Tripos Part IB. Part IB Paper 8: - ELECTIVE (2)

Engineering Tripos Part IB. Part IB Paper 8: - ELECTIVE (2) Engineering Tripos Part IB SECOND YEAR Part IB Paper 8: - ELECTIVE (2) MECHANICAL ENGINEERING FOR RENEWABLE ENERGY SYSTEMS Examples Paper 2 Wind Turbines, Materials, and Dynamics All questions are of Tripos

More information

Dynamics and Control of Rotorcraft

Dynamics and Control of Rotorcraft Dynamics and Control of Rotorcraft Helicopter Aerodynamics and Dynamics Abhishek Department of Aerospace Engineering Indian Institute of Technology, Kanpur February 3, 2018 Overview Flight Dynamics Model

More information

MODELING OF PLASMA ACTUATOR AND ITS EFFECT ON FLOW FIELD AROUND RECTANGULAR CYLINDER

MODELING OF PLASMA ACTUATOR AND ITS EFFECT ON FLOW FIELD AROUND RECTANGULAR CYLINDER Indian J.Sci.Res.1(2) : 803-814, 2014 ISSN : 0976-2876 (Print) ISSN : 2250-0138(Online) MODELING OF PLASMA ACTUATOR AND ITS EFFECT ON FLOW FIELD AROUND RECTANGULAR CYLINDER SAEED KAVOUSFAR a, HOSSEIN MAHDAVY-MOGHADDAM

More information

AERODYNAMIC COEFFICIENTS FOR EXTENDING AND BENDING PROJECTILES. William G. Reinecke*

AERODYNAMIC COEFFICIENTS FOR EXTENDING AND BENDING PROJECTILES. William G. Reinecke* 23 RD INTERNATIONAL SYMPOSIUM ON BALLISTICS TARRAGONA, SPAIN 16-20 APRIL 2007 AERODYNAMIC COEFFICIENTS FOR EXTENDING AND BENDING PROJECTILES William G. Reinecke* Institute for Advanced Technology.The University

More information

INSTITUTE OF AERONAUTICAL ENGINEERING (Autonomous) Dundigal, Hyderabad

INSTITUTE OF AERONAUTICAL ENGINEERING (Autonomous) Dundigal, Hyderabad INSTITUTE OF AERONAUTICAL ENGINEERING (Autonomous) Dundigal, Hyderabad - 500 043 AERONAUTICAL ENGINEERING TUTORIAL QUESTION BANK Course Name : LOW SPEED AERODYNAMICS Course Code : AAE004 Regulation : IARE

More information

Chapter 8 continued. Rotational Dynamics

Chapter 8 continued. Rotational Dynamics Chapter 8 continued Rotational Dynamics 8.4 Rotational Work and Energy Work to accelerate a mass rotating it by angle φ F W = F(cosθ)x x = s = rφ = Frφ Fr = τ (torque) = τφ r φ s F to s θ = 0 DEFINITION

More information

Fundamentals of Airplane Flight Mechanics

Fundamentals of Airplane Flight Mechanics David G. Hull Fundamentals of Airplane Flight Mechanics With 125 Figures and 25 Tables y Springer Introduction to Airplane Flight Mechanics 1 1.1 Airframe Anatomy 2 1.2 Engine Anatomy 5 1.3 Equations of

More information

Steps in the Finite Element Method. Chung Hua University Department of Mechanical Engineering Dr. Ching I Chen

Steps in the Finite Element Method. Chung Hua University Department of Mechanical Engineering Dr. Ching I Chen Steps in the Finite Element Method Chung Hua University Department of Mechanical Engineering Dr. Ching I Chen General Idea Engineers are interested in evaluating effects such as deformations, stresses,

More information

Influence of the Tooth Helix Angle on the Vibrations of a Cylindrical Gearbox

Influence of the Tooth Helix Angle on the Vibrations of a Cylindrical Gearbox Zoltan Korka, Ion Vela ANALELE UNIVERSITĂłII EFTIMIE MURGU REŞIłA ANUL XVI, NR. 1, 2009, ISSN 1453-7397 Influence of the Tooth Helix Angle on the Vibrations of a Cylindrical Gearbox The current trend in

More information

Mathematical Methods: Fourier Series. Fourier Series: The Basics

Mathematical Methods: Fourier Series. Fourier Series: The Basics 1 Mathematical Methods: Fourier Series Fourier Series: The Basics Fourier series are a method of representing periodic functions. It is a very useful and powerful tool in many situations. It is sufficiently

More information

NONLINEAR BEHAVIOR OF A SINGLE- POINT MOORING SYSTEM FOR FLOATING OFFSHORE WIND TURBINE

NONLINEAR BEHAVIOR OF A SINGLE- POINT MOORING SYSTEM FOR FLOATING OFFSHORE WIND TURBINE NONLINEAR BEHAVIOR OF A SINGLE- POINT MOORING SYSTEM FOR FLOATING OFFSHORE WIND TURBINE Ma Chong, Iijima Kazuhiro, Masahiko Fujikubo Dept. of Naval Architecture and Ocean Engineering OSAKA UNIVERSITY RESEARCH

More information

Finite Element Analysis of Piezoelectric Cantilever

Finite Element Analysis of Piezoelectric Cantilever Finite Element Analysis of Piezoelectric Cantilever Nitin N More Department of Mechanical Engineering K.L.E S College of Engineering and Technology, Belgaum, Karnataka, India. Abstract- Energy (or power)

More information

Introduction to Continuous Systems. Continuous Systems. Strings, Torsional Rods and Beams.

Introduction to Continuous Systems. Continuous Systems. Strings, Torsional Rods and Beams. Outline of Continuous Systems. Introduction to Continuous Systems. Continuous Systems. Strings, Torsional Rods and Beams. Vibrations of Flexible Strings. Torsional Vibration of Rods. Bernoulli-Euler Beams.

More information

ARC241 Structural Analysis I Lecture 5, Sections ST4.5 ST4.10

ARC241 Structural Analysis I Lecture 5, Sections ST4.5 ST4.10 Lecture 5, Sections ST4.5 ST4.10 ST4.5) Moment of a Force about a Specified Axis ST4.6) Moment of a Couple ST4.7) Equivalent System ST4.8) Resultant of a Force and a Couple System ST4.9) Further Reduction

More information

Tuesday, February 11, Chapter 3. Load and Stress Analysis. Dr. Mohammad Suliman Abuhaiba, PE

Tuesday, February 11, Chapter 3. Load and Stress Analysis. Dr. Mohammad Suliman Abuhaiba, PE 1 Chapter 3 Load and Stress Analysis 2 Chapter Outline Equilibrium & Free-Body Diagrams Shear Force and Bending Moments in Beams Singularity Functions Stress Cartesian Stress Components Mohr s Circle for

More information

AXTRUSION SUPPLEMENTARY MATERIALS. An approximate formula for estimating a bearing s stiffness is 1. P s A 2 h

AXTRUSION SUPPLEMENTARY MATERIALS. An approximate formula for estimating a bearing s stiffness is 1. P s A 2 h Appendix A AXTRUSION SUPPLEMENTARY MATERIALS A. Carriage Stiffness Estimates This section describes the steps to predict the stiffness performance of the carriage. First an accurate stiffness model of

More information

A STUDENT'S INTRODUCTION TO THE WRIGHT BROTHERS WIND TUNNEL AT MIT. Eugene E. Covert T. Wilson Professor Emeritus INTRODUCTION

A STUDENT'S INTRODUCTION TO THE WRIGHT BROTHERS WIND TUNNEL AT MIT. Eugene E. Covert T. Wilson Professor Emeritus INTRODUCTION A STUDENT'S INTRODUCTION TO THE WRIGHT BROTHERS WIND TUNNEL AT MIT Eugene E. Covert T. Wilson Professor Emeritus INTRODUCTION A wind tunnel is an instrument whose purpose is to measure some aerodynamic

More information

Use of Microspoilers for Control of Finned Projectiles

Use of Microspoilers for Control of Finned Projectiles JOURNAL OF SPACECRAFT AND ROCKETS Vol., No. 6, November December Use of Microspoilers for Control of Finned Projectiles Downloaded by GEORGIA INST OF TECHNOLOGY on February 7, 3 http//arc.aiaa.org DOI.5/.6

More information

Bluff Body, Viscous Flow Characteristics ( Immersed Bodies)

Bluff Body, Viscous Flow Characteristics ( Immersed Bodies) Bluff Body, Viscous Flow Characteristics ( Immersed Bodies) In general, a body immersed in a flow will experience both externally applied forces and moments as a result of the flow about its external surfaces.

More information

Introduction to Flight Dynamics

Introduction to Flight Dynamics Chapter 1 Introduction to Flight Dynamics Flight dynamics deals principally with the response of aerospace vehicles to perturbations in their flight environments and to control inputs. In order to understand

More information

D : SOLID MECHANICS. Q. 1 Q. 9 carry one mark each.

D : SOLID MECHANICS. Q. 1 Q. 9 carry one mark each. GTE 2016 Q. 1 Q. 9 carry one mark each. D : SOLID MECHNICS Q.1 single degree of freedom vibrating system has mass of 5 kg, stiffness of 500 N/m and damping coefficient of 100 N-s/m. To make the system

More information

inter.noise 2000 The 29th International Congress and Exhibition on Noise Control Engineering August 2000, Nice, FRANCE

inter.noise 2000 The 29th International Congress and Exhibition on Noise Control Engineering August 2000, Nice, FRANCE Copyright SFA - InterNoise 2000 1 inter.noise 2000 The 29th International Congress and Exhibition on Noise Control Engineering 27-30 August 2000, Nice, FRANCE I-INCE Classification: 1.1 DESIGN OF TERMINATING

More information

ME 101: Engineering Mechanics

ME 101: Engineering Mechanics ME 0: Engineering Mechanics Rajib Kumar Bhattacharja Department of Civil Engineering ndian nstitute of Technolog Guwahati M Block : Room No 005 : Tel: 8 www.iitg.ernet.in/rkbc Area Moments of nertia Parallel

More information

3.0 FINITE ELEMENT MODEL

3.0 FINITE ELEMENT MODEL 3.0 FINITE ELEMENT MODEL In Chapter 2, the development of the analytical model established the need to quantify the effect of the thermal exchange with the dome in terms of a single parameter, T d. In

More information

Dynamics Plane kinematics of rigid bodies Section 4: TJW Rotation: Example 1

Dynamics Plane kinematics of rigid bodies Section 4: TJW Rotation: Example 1 Section 4: TJW Rotation: Example 1 The pinion A of the hoist motor drives gear B, which is attached to the hoisting drum. The load L is lifted from its rest position and acquires an upward velocity of

More information

Experimental Studies on Complex Swept Rotor Blades

Experimental Studies on Complex Swept Rotor Blades International Journal of Engineering Research and Technology. ISSN 974-3154 Volume 6, Number 1 (213), pp. 115-128 International Research Publication House http://www.irphouse.com Experimental Studies on

More information

AP Unit 8: Uniform Circular Motion and Gravity HW

AP Unit 8: Uniform Circular Motion and Gravity HW Basics 1D Mot. 2D Mot. Forces Energy Moment. Rotation Circ/Grav SHM Waves Circuits AP Unit 8: Uniform Circular Motion and Gravity HW AP Exam Knowledge & Skills (What skills are needed to achieve the desired

More information

Thermal Field in a NMR Cryostat. Annunziata D Orazio Agostini Chiara Simone Fiacco

Thermal Field in a NMR Cryostat. Annunziata D Orazio Agostini Chiara Simone Fiacco Thermal Field in a NMR Cryostat Annunziata D Orazio Agostini Chiara Simone Fiacco Overall Objective of Research Program The main objective of the present work was to study the thermal field inside the

More information

Name: Fall 2014 CLOSED BOOK

Name: Fall 2014 CLOSED BOOK Name: Fall 2014 1. Rod AB with weight W = 40 lb is pinned at A to a vertical axle which rotates with constant angular velocity ω =15 rad/s. The rod position is maintained by a horizontal wire BC. Determine

More information

Item Descriptions Developed During the TIMSS Advanced 2008 Benchmarking

Item Descriptions Developed During the TIMSS Advanced 2008 Benchmarking Item Descriptions Developed During the TIMSS Advanced 2008 Benchmarking Advanced Mathematics Items at Intermediate International Benchmark (475) Algebra M2_01 M6_02 Rationalizes the denominator in an expression

More information

Solving Direct and Inverse Heat Conduction Problems

Solving Direct and Inverse Heat Conduction Problems Solving Direct and Inverse Heat Conduction Problems Jan Taler Piotr Duda Solving Direct and Inverse Heat Conduction Problems ~ Springer Preface This book is devoted to the concept of simple and inverse

More information

Chapter 2 HEAT CONDUCTION EQUATION

Chapter 2 HEAT CONDUCTION EQUATION Heat and Mass Transfer: Fundamentals & Applications 5th Edition in SI Units Yunus A. Çengel, Afshin J. Ghajar McGraw-Hill, 2015 Chapter 2 HEAT CONDUCTION EQUATION Mehmet Kanoglu University of Gaziantep

More information

Experimental Investigation of the Aerodynamic Forces and Pressures on Dome Roofs: Reynolds Number Effects

Experimental Investigation of the Aerodynamic Forces and Pressures on Dome Roofs: Reynolds Number Effects Experimental Investigation of the Aerodynamic Forces and Pressures on Dome Roofs: Reynolds Number Effects *Ying Sun 1), Ning Su 2), Yue Wu 3) and Qiu Jin 4) 1), 2), 3), 4) Key Lab of Structures Dynamic

More information

Flight Vehicle Terminology

Flight Vehicle Terminology Flight Vehicle Terminology 1.0 Axes Systems There are 3 axes systems which can be used in Aeronautics, Aerodynamics & Flight Mechanics: Ground Axes G(x 0, y 0, z 0 ) Body Axes G(x, y, z) Aerodynamic Axes

More information

SILVER OAK COLLEGE OF ENGINEERING & TECHNOLOGY ADITYA SILVER OAK INSTITUTE OF TECHNOLOGY

SILVER OAK COLLEGE OF ENGINEERING & TECHNOLOGY ADITYA SILVER OAK INSTITUTE OF TECHNOLOGY SUBJECT: ENGINEERING THERMODYNAMICS (2131905) (ME) DATE: 11-08-2017 TIME: 10:00 am to 11:30 am TOTAL MARKS: 40 Q.1 (a) Answer following questions in short/brief: 1. Energy of an isolated system is always

More information

Optimal Design of PM Axial Field Motor Based on PM Radial Field Motor Data

Optimal Design of PM Axial Field Motor Based on PM Radial Field Motor Data Optimal Design of PM Axial Field Motor Based on PM Radial Field Motor Data GOGA CVETKOVSKI LIDIJA PETKOVSKA Faculty of Electrical Engineering Ss. Cyril and Methodius University Karpos II b.b. P.O. Box

More information

Chapter 8 continued. Rotational Dynamics

Chapter 8 continued. Rotational Dynamics Chapter 8 continued Rotational Dynamics 8.4 Rotational Work and Energy Work to accelerate a mass rotating it by angle φ F W = F(cosθ)x x = rφ = Frφ Fr = τ (torque) = τφ r φ s F to x θ = 0 DEFINITION OF

More information

Chapter 2 HEAT CONDUCTION EQUATION

Chapter 2 HEAT CONDUCTION EQUATION Heat and Mass Transfer: Fundamentals & Applications Fourth Edition Yunus A. Cengel, Afshin J. Ghajar McGraw-Hill, 2011 Chapter 2 HEAT CONDUCTION EQUATION Mehmet Kanoglu University of Gaziantep Copyright

More information