PPT-Rigid body rotation

Physics 7C lecture 13 Tuesday November 12 800 AM 920 AM Engineering Hall 1200 Applying a torque Torque τ r F Torque and angular acceleration for a rigid body The rotational analog of Newton. 5. Finite Element Analysis of Contact Problem. Nam-Ho Kim. Goals. Learn the computational difficulty in boundary nonlinearity. Understand the concept of variational inequality and its relation with the constrained optimization. Rigid Body Simulation. The . next. . few. . lectures. …. Comming. . up. …. Dynamic simulation . Movement of point masses, rigid bodies, systems of point masses etc. with respect to. Forces . Body charcteristics (mass, shape). A Comprehensive Introduction. Motivation. Motiviation. Rigid Body Motion is all around us. Rigid Body Motion is . the. game physics concept in use. Bullet, . Havok. , ODE all use this concept. You. need to know about it if you want to work with and understand physics engines!. Rigid Transformations. 3D Rigid Objects. Rigid Transformation in 2D. q = (. t. x. ,t. y. ,. q. ) . with . q. . . [0,2. p. ). Robot R. 0. . R. 2. given in reference frame T. 0. What’s the new robot . Warm Up. U. se the points G(-3, -7) and H(2, -3) to answer the following:. 1.. Find the slope of . 2. . Find the midpoint of . 3. . Find GH.  . Objectives. 1.4 Transformations. Identify reflections, rotations, and translations. . Dedra. Demaree, . Georgetown University. © 2014 Pearson Education, Inc.. Rotational Motion. How can a star rotate 1000 times faster than a merry-go-round?. Why is it more difficult to balance on a stopped bike than on a moving bike?. Motivation. Motiviation. Rigid Body Motion is all around us. Rigid Body Motion is . the. game physics concept in use. Bullet, . Havok. , ODE all use this concept. You. need to know about it if you want to work with and understand physics engines!. Dynamics of Planar Systems. November 08, 2011. 6.1.3, 6.1.4, 6.2, starting 6.3. © Dan Negrut, . 2011. ME451, UW-Madison. TexPoint fonts used in EMF. . Read the TexPoint manual before you delete this box.: . Rigid Transformations. 3D Rigid Objects. Rigid Transformation in 2D. q = (. t. x. ,t. y. ,. q. ) . with . q. . . [0,2. p. ). Robot R. 0. . R. 2. given in reference frame T. 0. What’s the new robot . Quiz – You are building a house and there is a door mounted on hinges. Where do you put the door knob?. On the edge of the door near the hinges. On the edge of the door away from the hinges. On the middle of the door.. What is this plane? What halves do you get? . What is this plane? What halves do you get? . 1. 2. 3. Remember: for a movement to occur in a plane, it must be parallel with that plane!. What are the 2 opposing . Aeroservoelastic. Workshop. NASA Langley Research Center. Jeff Beranek. MAD Deputy Program Manager. John Scarcello. Research Engineering Manager. April 18-19, 2012. Create and Deliver Superior Products Through Innovative Minds. Erich Ritz and P. C. Chen. 9489 E. Ironwood Square Drive, Scottsdale, AZ 85258, Tel. (480) 945-9988, Fax (480) 945-6588, E-mail: info@zonatech.com . Presented at ASE Workshop, NASA Langley, VA on April 18-19, 2012. 4 - . 2. Equilibrium of a Rigid Body in Three Dimensions. Six scalar equations are required to express the conditions for the equilibrium of a rigid body in the general three dimensional case..  .