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ME375 System Modeling and Analysis

ME375 System Modeling and Analysis. Rotational Mechanical Systems. Rotational Mechanical Systems. Variables Basic Modeling Elements Interconnection Laws Derive Equation of Motion (EOM). J. q. K. t ( t ). B. Variables. q : angular displacement [rad] w : angular velocity [rad/sec].

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ME375 System Modeling and Analysis

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  1. ME375 System Modeling and Analysis Rotational Mechanical Systems

  2. Rotational Mechanical Systems • Variables • Basic Modeling Elements • Interconnection Laws • Derive Equation of Motion (EOM)

  3. J q K t (t) B Variables • q : angular displacement [rad] • w: angular velocity [rad/sec] • a: angular acceleration [rad/sec2] • t: torque [Nm] • p : power [Nm/sec] • w : work ( energy ) [Nm] 1 [Nm] = 1 [J] (Joule)

  4. Basic Rotational Modeling Elements • Damper • Friction Element • Analogous to Translational Damper. • Dissipate Energy. • E.g. bearings, bushings, ... • Spring • Stiffness Element • Analogous to Translational Spring. • Stores Potential Energy. • E.g. shafts tD tD tS B tS q1 q2

  5. d Basic Rotational Modeling Elements • Parallel Axis Theorem • Ex: • Moment of Inertia • Inertia Element • Analogous to Mass in Translational Motion. • Stores Kinetic Energy.

  6. Interconnection Laws • Newton’s Second Law • Newton’s Third Law • Action & Reaction Torque • Lever (Motion Transformer Element) Massless or small acceleration

  7. Motion Transformer Elements • Rack and Pinion • Gears Ideal case Gear 1 Gear 2

  8. J q K t (t) B Example Derive a model (EOM) for the following system: FBD: (Use Right-Hand Rule to determine direction) J K B

  9. Energy Distribution • EOM of a simple Mass-Spring-Damper System We want to look at the energy distribution of the system. How should we start ? • Multiply the above equation by angular velocity termw : Ü What have we done ? • Integrate the second equation w.r.t. time:Ü What are we doing now ?

  10. J q K t (t) B Energy Method • Change of energy in system equals to net work done by external inputs • Change of energy in system per unit time equals to net power exerted by external inputs • EOM of a simple Mass-Spring-Damper System

  11. Rolling without slipping FBD: Elemental Laws: x x q q fs f(t) fd Mg ff N Example Coefficient of friction m K R B f(t) J, M Kinematic Constraints: (no slipping)

  12. Example (cont.) I/O Model (Input: f, Output: x): Q: How would you decide whether or not the disk will slip? If Slipping happens. Q: How will the model be different if the disk rolls and slips ? does not hold any more

  13. Rolling without slipping Kinetic Energy x q Example (Energy Method) Power exerted by non-conservative inputs Coefficient of friction m K R B f(t) Energy equation J, M Kinematic Constraints: (no slipping) Potential Energy EOM

  14. Example (coupled translation-rotation) Real world Think about performance of lever and gear train in real life

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