Subject Name: Dynamics of Machines Subject Code: 10AE53

Slides:



Advertisements
Similar presentations
Engine Geometry BC L TC l VC s a q B
Advertisements

Mechatronics Simulation Project IC Engine – Power Cylinder Modeling Anthony R. Copp E579 - Mechatronic Modeling Spring 2006.
MSTC Physics Chapter 8 Sections 3 & 4.
Chapter 9 Rotational Dynamics. 9.5 Rotational Work and Energy.
Internal Combustion Engine Testing
CTC / MTC 222 Strength of Materials Chapter 5 Torsional Shear Stress and Torsional Deformation.
College and Engineering Physics Quiz 8: Rotational Equations and Center of Mass 1 Rotational Equations and Center of Mass.
D. Roberts PHYS 121 University of Maryland Physic² 121: Phundament°ls of Phy²ics I December 11, 2006.
CTC / MTC 222 Strength of Materials
Chapter 11 Rotational Dynamics and Static Equilibrium
Dr. Ali Al-Gadhib 1)To find the relationship between torque and the amount of power delivered to rotate a shaft. 2)To design a shaft to carry a given power.
BTE 1013 ENGINEERING SCIENCEs
L ESSON 5: M ECHANICS FOR M OTORS AND G ENERATORS ET 332a Dc Motors, Generators and Energy Conversion Devices 1.
Reciprocating Compressor
TRANSMISSION SYSTEM (GEAR BOX)
MAE 242 Dynamics – Section I Dr. Kostas Sierros.
Angular Momentum of a Particle
C O B A w=2 rad/s 2 m a=4 rad/s2 PROBLEMS
Sub unit 6.1 ”Power in Mechanical Systems”
§ 7 - 1 Introduction § 7 - 2 Motion Equation of a Mechanical System § 7 - 5 Introduction to Aperiodic speed Fluctuation and Its Regulation § 7 - 4 Periodic.
G.K.BHARAD INSTITUTE OF ENGINEERING Group :03 G.K.BHARAD INSTITUTE OF ENGINEERING Subject : Element Of Mechanical Engineering Subject Code : Topic.
Q10. Rotational Motion.
 Energy is the capacity of doing work.  Energy methods are useful in analyzing machines that store energy. counterweights springs flywheels Energy Methods.
DYNAMICS OF ELECTRIC DRIVES
Newton’s Second Law for Rotation Examples 1.The massive shield door at the Lawrence Livermore Laboratory is the world’s heaviest hinged door. The door.
Physics 111 Practice Problem Statements 09 Rotation, Moment of Inertia SJ 8th Ed.: Chap 10.1 – 10.5 Contents 11-4, 11-7, 11-8, 11-10, 11-17*, 11-22, 11-24,
NAZARIN B. NORDIN What you will learn: Simple machines Mechanical advantage (force ratio) Movement ratio (velocity ratio) Machine.
Rotational Dynamics Chapter 8 Section 3.
EET 421 POWER ELECTRONIC DRIVES. Motor drive systems definitions Review of motor principles Mechanical Requirements of Motor Drives.
Chapter Angular Position, Velocity, and Acceleration 10.2
Simple Harmonic Motion: SHM
Physics. Session Rotational Mechanics - 1 Session Opener Earth rotates about its own axis in one day. Have you ever wondered what will happen to the.
Sci 701 Unit 5 Speed is a measure of how fast an object is moving, that is, how much distance it will travel over a given time. This measure is given.
Rotational Dynamics 8.3. Newton’s Second Law of Rotation Net positive torque, counterclockwise acceleration. Net negative torque, clockwise acceleration.
Physics. Session Rotational Mechanics - 3 Session Objectives.
THOERY OF MECHANISMS AND MACHINES Module-12 ENGINE DYNAMICS, BALANCING INLINE ENGINES FLYWHEELS, BELT-PULLEY DRIVES Instructed by: Dr. Anupam Saxena Associate.
Teaching Innovation - Entrepreneurial - Global
FLUID POWER CONTROL ME604C.
Rotation of a Rigid Object About a Fixed Axis 10.
FLYWHEEL Prepare By: – Raninga Raj
Rotational Mechanics 1 We know that objects rotate due to the presence of torque acting on the object. The same principles that were true for what caused.
FLYWHEEL Made by: AADITYA A PATEL
Phys211C10 p1 Dynamics of Rotational Motion Torque: the rotational analogue of force Torque = force x moment arm  = Fl moment arm = perpendicular distance.
Flywheel Darshan Baru Prepared By: Darshan Baru Bhanushali Deep Milind Bhoya Theory of Machine.
AHMEDABAD INSTITUTE OF TECHNOLOGY. TOPIC: RECIPROCATING PUMPS NAME: (1)SAKARIYA BRIJESH ( ) (2)RAVAL JAINIL ( ) (3)RAVAL YASH ( )
Simple Harmonic Motion
Turning Moment Diagram
Mechanical Vibrations
FLYWHEEL (PSG Design Data Book p: ).
Balancing of Reciprocating Masses
Lesson 6: Mechanics for Motors and Generators
GOVERNOR Prepare By: – Korat Parth
M 97 b b M P a a M 1. Find the moment of inertia around P
Darshan institute of engineering & technology
Visit for more Learning Resources
Physics 111 Exam 2 and part of 3 Review.
9/16/2018 Physics 253.
Subject Name: Dynamics of Machines Subject Code: 10AE53
Subject Name: Dynamics of Machines Subject Code: 10AE53
Assignments cont’d… 1. Determine
Subject Name: Dynamics of Machines Subject Code: 10AE53
Subject Name: Dynamics of Machines Subject Code: 10AE53
WEEKS Dynamics of Machinery
WEEK 4 Dynamics of Machinery
Torque & Angular Acceleration AH Physics
Utilisation of Electrical Energy
A solid cylinder with a radius of 4
DYNAMICS OF MACHINERY Presented by E LAKSHMI DEVI M.Tech,
Dynamics of Machinery Problems and Solutions
Presentation transcript:

Subject Name: Dynamics of Machines Subject Code: 10AE53 Prepared By: A.Amardeep Department: Aeronautical Eng.. Date: 25-08-2014 11/24/2018

Dynamic Force Analysis and Turning Moment Diagrams and Flywheel Topic details Dynamic Force Analysis and Turning Moment Diagrams and Flywheel 11/24/2018

Introduction The turning moment diagram (also known as crank effort diagram) is the graphical representation of the turning moment or crank-effort for various positions of the crank. It is plotted on Cartesian co-ordinates, in which the turning moment is taken as the ordinate and crank angle as abscissa. 11/24/2018

Cond.. Turning Moment Diagram for a Single Cylinder Double Acting Steam Engine 11/24/2018

Turning Moment Diagram for a Four Stroke Cycle Internal Combustion Engine 11/24/2018

Turning Moment Diagram for a Multi-cylinder Engine 11/24/2018

Flywheel A flywheel used in machines serves as a reservoir, which stores energy during the period when the supply of energy is more than the requirement, and releases it during the period when the requirement of energy is more than the supply. In other words, a flywheel controls the speed variations caused by the fluctuation of the engine turning moment during each cycle of operation. 11/24/2018

Cond.. 11/24/2018

11/24/2018

Cond.. 11/24/2018

Flywheels as energy reservoir : Crank pin brg Crank shaft F L Y W H E Main brgs 11/24/2018

Example : ( flywheel calculation ) The torque exerted on the crank of a two stroke engine Is given as T ( ) = [15,000+2,000sin 2() – 1,800cos 2()] N.m If the load torque on the engine is constant, Determine the following : 1.Power of the engine if the mean speed is 150 rpm. 2.M.I of the flywheel if Ks =0.01 3.Angular acceleration of the flywheel for  =30 o 11/24/2018

 T-  diagram of the example problem T T, T r=Ta =15,000N.m 1= 21o E max 13,200 1= 21o  2 = 111o 11/24/2018

= 1 /2 ∫0 2 (15000+2000sin 2() - 1800cos 2()) d Solution : T av = 1 /2 ∫0 2 M d = 1 /2 ∫0 2 (15000+2000sin 2() - 1800cos 2()) d = 15,000 N.m = T r ( resisting torque) Work output /cycle = (15,000 X 2 ) N.m Work output /second = 15,000 X 2 ( 150 /60 ) W Power of the engine = 235.5 k W 11/24/2018

The value of  at which T- diagram intersect with T r are given by [15000+2000sin 2() - 1800cos 2()] = 15,000 N.m or [2000sin 2() - 1800cos 2()] = 0,  tan2 =0.9 2()1 = 42o & 2()2 = (180+ 42)o ()1 = 21o & ()2 = 111o E max = ∫ ()1 () 2( 2000sin 2() - 1800cos 2()) d = 2690.2 N.m Contd…. 11/24/2018

Using the relation , E max = I 2 Ks We have Ks = 0.01 &  = (150 X 2)/ 60 =15.7 rad /s Using the relation , E max = I 2 Ks M.I of the flywheel , I = 2690.2 / (15.7 2 X 0.01) = 1090 kg.m2 when  = 30o , T = 15,000+ 1732 -900 = 15,832 N.m Hence ang. acceleration of the flywheel at  = 30o  30 = (15,832 -15,000) / 1090 = 0.764 rad /s2 11/24/2018

Flywheels of punching presses: Prime mover shaft torque Load torque Reciprocating varying torque constant Engine Electrical constant varying torque Motors for Press operation 11/24/2018

 r (2- 1) / 2  = t / 2 s = t / 4 r t tool IDC job T- diagram of press Peak torque 1 2 machine torque  r Motor torque 1 2  tool Assuming uniform velocity of the tool, (2- 1) / 2  = t / 2 s = t / 4 r t IDC job 11/24/2018

Operation :3.8 cm dia hole in 3.2 cm plate Example : Operation :3.8 cm dia hole in 3.2 cm plate Work done in punching : 600 N.m / cm2 of sheared area Stroke of the punch : 10.2 cm No. of holes punched : 6 holes /min Max speed of the flywheel at its rg = 27.5 m /s Min speed of the flywheel at its rg = 24.5 m /s To find : Power of the motor of the machine ? Mass of the required flywheel ? 11/24/2018

Sheared area /hole =  d t =  X 3.8 X 3.2 = 38.2 cm2 Solution : Sheared area /hole =  d t =  X 3.8 X 3.2 = 38.2 cm2  work done in shearing /hole = 38.2 X 600 = 22,920 N.m  work done / minute = (22,920 X 6) N.m Power of the motor = (22,920 X 6) / 60 = 2.292 k W We have, t /2s = 3.2 / (2 X 10.2) =3.2 / 20.4= (2- 1) / 2  Energy required by the machine / cycle = 22,920 N.m Energy delivered by the motor during actual Punching i.e ( when crank rotates from 1 to 2 ) = 22,920 X ( t /2s ) = 22,920 X (3.2 /20.4) = 3,595 N.m Contd … 11/24/2018

Max .fluctuation of energy, E max = 22,920- 3595 =19,325 N.m = m rg2 ( 12 - 22 ) / 2 But rg2 12 = 27.5 m/s & rg2 22 = 24.5 m/s  m ( 27.5 2 -24.5 2) / 2 = 19,325 m = 244 k g 11/24/2018

11/24/2018