Survey
* Your assessment is very important for improving the workof artificial intelligence, which forms the content of this project
* Your assessment is very important for improving the workof artificial intelligence, which forms the content of this project
Elementary particle wikipedia , lookup
Specific impulse wikipedia , lookup
Newton's laws of motion wikipedia , lookup
Rigid body dynamics wikipedia , lookup
Modified Newtonian dynamics wikipedia , lookup
Mass in special relativity wikipedia , lookup
Seismometer wikipedia , lookup
Atomic theory wikipedia , lookup
Electromagnetic mass wikipedia , lookup
Topic 2.1 Extended N – Center of mass 1 Up to this point we've considered only "point masses" which can be treated as if they have no "extent." The reason we do this is so that we can treat all of the particles in the mass as one - all having the same position, speed and acceleration. Even if the mass is extended, as in this wrench, we can treat it as a point mass as long as it is not rotating. If the wrench is rotating as it slides, we can no longer treat it as a point mass: Note that of all of the points on the extended body, ONLY THE WHITE DOT FOLLOWS A STRAIGHT LINE. We call the position of the white dot the center of mass. The center of mass (CM) is that point about which all other points of the extended mass rotate (if rotation even occurs). This section will teach you how to find the center of mass of an extended body. We'll need this skill later when we look at rotation, and balancing structures. Topic 2.1 Extended N – Center of mass 1 It turns out that if you have an extended mass, Newton's 2nd law applies to the center of mass (cm) of the extended mass: We write Fnet, external = MAcm Newton's 2nd Law for a System of Particles where M is the total mass of the extended mass. Note that only the external force contributes to the acceleration of the system. Since the spreading explosion of the fireworks was caused by internal forces, the whole mass will continue along the original parabolic trajectory: Topic 2.1 Extended N – Center of mass 1 Since Acm = Vcm , we can write t Fnet, external = MAcm Vcm Fnet, external = M t MVcm Fnet, external = t Newton's 2nd Law Fnet, external = P t P-form where P = MVcm is the total momentum of the system of particles making up the extended mass. If Fnet, external = 0 then we see that P = MVcm is zero. FYI: Thus, if the net external force acting on a system of particles is ZERO, that cm of that system must move at a constant velocity or be at rest. FYI: The cm is where we can think of all the mass of an extended Topic 2.1 Extended body as being concentrated as far as translational motion is concerned. N – Center of mass 1 CENTER OF MASS The center of mass is applicable to ANY system of masses - even those of a gas. particles we have Xcm = For a system of n m1x1 + m2x2 + ... + mnxn m1 + m2 + ... + mn n Xcm = mixi M Location of Xcm i= 1 Find the center of mass of the following system: 3 kg 2 kg y 8 kg 1 kg x m1x1 + m2x2 + m3x3 + m4x4 m1 + m2 + m3 + m4 3-7 + 2-2 + 80 + 17 = 3 + 2 + 8 + 1 xcm = = -1.3 m Topic 2.1 Extended N – Center of mass 1 CENTER OF MASS The center of mass doesn't necessarily have to lie within the mass itself. n (xcm,ycm) Ycm (xcm,ycm) n (xcm,ycm,zcm) Zcm = mizi M i= 1 miyi i= 1 = M FYI: The cg is now known, but a third trial will ensure that our first two mappings are correct:Topic 2.1 Extended N –directly Center ofpoint mass 1 FYI: The cg must hang below the of suspension at the tip of Albert's tail. Albert is playing "dead" for this experiment, and so is CENTER OFstiff. GRAVITY completely The center of gravity (CG) is where we can think of the weight of an extended body to be concentrated as far as translational motion is concerned. In a region where g is constant, the CG can be found from n Xcg m gx = i= 1 i i Mg Location of Xcg How would you find the CG of Albert? Albert the physics cat Since Albert is asymmetric, you find his center of gravity by hanging him three different ways: