Rotating Frames of Reference and the Vector Concept

1960 ◽  
Vol 67 (10) ◽  
pp. 976-982
Author(s):  
Robert C. Wrede
Author(s):  
Deep Bhattacharjee ◽  
Deep Bhattacharjee

Comment: Time itself being the temporal dimensions can be manipulated by means of clever physics so as to make a time travelling domain in the backyard of your own garden. The principles of this are introduced along with physics, so as to capture the beauty of time travelling on a grander scale by some arbitrarily modified civilizations in the faraway futures. This starts with the basic notions on the perspectives of time with regards to its implications in the physics of the time travel.


1960 ◽  
Vol 67 (10) ◽  
pp. 976
Author(s):  
Robert C. Wrede

2017 ◽  
Vol 29 (33) ◽  
pp. 1700614 ◽  
Author(s):  
Konrad Giżynski ◽  
Taehoon Lee ◽  
Bartosz A. Grzybowski

1979 ◽  
Vol 12 (9) ◽  
pp. 1425-1440 ◽  
Author(s):  
D G Ashworth ◽  
P A Davies

Author(s):  
Karuna Koppula ◽  
Andre´ Be´nard ◽  
Charles Petty

In rotating homogeneous decay, the prolate quadratic form associated with the normalized Reynolds (NR-) stress is elongated by a coupling between velocity fluctuations and the Coriolis acceleration. This paper shows that this well-known turbulence phenomenon is consistent with an algebraic anisotropic prestress (APS-) closure for the NR-stress that unifies the study of turbulent flows in rotating and non-rotating frames-of-reference. The APS-closure is a non-negative mapping of the NR-stress into itself and is, thereby, universally realizable for all turbulent flows.


1996 ◽  
Vol 118 (4) ◽  
pp. 606-613 ◽  
Author(s):  
M. W. D. White ◽  
G. R. Heppler

Timoshenko beam theory is used to model a flexible slewing link with an attached payload using two different rotating frames of reference: pseudo-pinned and pseudo-clamped. The boundary conditions are presented for both formulations; these lead naturally to the frequency equation for the link. The infinite dimensional model of the slewing link is then approximated by a finite dimensional model. Finally, these two formulations are shown to be equivalent through a simple transformation.


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