 ... energy as part of their thermal energy. The view therefore is plausible that the emission and absorption of radiant energy in band spectra represent changes in this rotational energy. If molecules were really rigid bodies, the application of Bohr's...  A Treatise on Gyrostatics and Rotational Motion - Page 415by Andrew Gray - 1918 - 530 pagesFull view - About this book
 | Royal Society of Edinburgh - Science - 1909 - 834 pages
...with this we have the kinetic energy of rotation Tr = i{A(£ + #sin*0) + C(^ + «£cose)2} . . . (55); where C is the moment of inertia of the body about...symmetry and passing through the centroid. Then T = Tr + T ....... (56). 27. It will be seen from an examination of the expression for T above, that... | |
 | Royal Society of Edinburgh - Science - 1909 - 886 pages
...we have the kinetic energy of rotation Tr = J{ A(02 + # sin2 0) + C(«£ + <£ oosfl)2} . . . (55); where C is the moment of inertia of the body about...symmetry and passing through the centroid. Then T = Tf + Tr (56). 27. It will be seen from an examination of the expression for T above, that the mtegrability... | |
 | William Suddards Franklin, Barry MacNutt - Heat - 1910 - 432 pages
...momentum or spin momentum of the body, that is to say, the spin momentum of a body is equal to Ku, where K is the moment of inertia of the body about its axis of spin, and co is its spin velocity in radians per second. The spin momentum of a body cannot change... | |
 | Louis Adolphe Martin - Mechanics - 1912 - 244 pages
...and v the velocity of its mass-center. The kinetic energy of a rotating body is /CO2 — , 2 where / is the moment of inertia of the body about its axis of rotation and co is the angular velocity of the body about the same axis. The moment of inertia of a... | |
 | Alonzo Morris Buck - Electric railroads - 1915 - 412 pages
...rotation, its moment is pBdM XP = p*edM The total moment of the whole rotating mass is = K9 (14) where K is the moment of inertia of the body about its axis of rotation. It may also be expressed by the relation K = fc2M (15) where A; is the radius of gyration... | |
 | Norman Robert Campbell - Atoms - 1921 - 128 pages
...were really rigid bodies, the application of Bohr's principles to the suggestion would be simple. If / is the moment of inertia of the body about its axis of rotation, to the angular velocity of rotation, the energy of rotation is given by W= \Iuf' (106). 1... | |
 | Norman Robert Campbell - 128 pages
...were really rigid bodies, the application of Bohr's principles to the suggestion would be simple. If / is the moment of inertia of the body about its axis of rotation, to the angular velocity of rotation, the energy of rotation is given by W =\Ia? (106). 1... | |
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