
Centre de Recerca Matem`atica
... This is a very important notion in foliation theory. To make it clear, let us give the main examples of such structures. 2.2. Lie foliations We say that F is a Lie G-foliation, if T is a Lie group G and γij are restrictions of left translations on G. Such foliation can also be defined by a 1-form ω ...
... This is a very important notion in foliation theory. To make it clear, let us give the main examples of such structures. 2.2. Lie foliations We say that F is a Lie G-foliation, if T is a Lie group G and γij are restrictions of left translations on G. Such foliation can also be defined by a 1-form ω ...
Realizing nonholonomic dynamics as limit of friction forces
... body rigid. Finally, a smooth, convex body rolling on a surface without slipping, or a figure skater sliding without sideways movement are examples of the idealization of friction forces, and modeled by nonholonomic mechanics. The examples above show how both holonomically and nonholonomically const ...
... body rigid. Finally, a smooth, convex body rolling on a surface without slipping, or a figure skater sliding without sideways movement are examples of the idealization of friction forces, and modeled by nonholonomic mechanics. The examples above show how both holonomically and nonholonomically const ...
Acceleration Analysi..
... felt on our feet or buttocks, is defined by our mass times the acceleration due to gravity or mg. Thus an imposed acceleration of 1 g above the baseline of our gravity, or 2 g's, will be felt as a doubling of our weight. At 6 g's we would feel six times as heavy as normal and would have great diffic ...
... felt on our feet or buttocks, is defined by our mass times the acceleration due to gravity or mg. Thus an imposed acceleration of 1 g above the baseline of our gravity, or 2 g's, will be felt as a doubling of our weight. At 6 g's we would feel six times as heavy as normal and would have great diffic ...