1987
DOI: 10.1119/1.14997
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Trouble on the loop-the-loop

Abstract: Energy considerations give an incorrect value for the minimum height from which a sphere may be released on the approach track of a loop-the-loop, assuming that the sphere rolls without slipping. Analytical and graphical methods are described for predicting whether the sphere will negotiate the top of the circular loop for arbitrary conditions of release height and coefficients of friction. Finally, a situation in which a sphere commences to slip immediately upon release is discussed.

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Cited by 5 publications
(4 citation statements)
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“…It can be concluded that when the velocity v 0 is below the threshold value in equation ( 27), the sphere cannot complete the vertical loop rolling without slipping in all points of the path. Following another formulation, Tea [7] also concludes that according to the conventional solution of the classical problem (h = 2.7R), the static friction coefficient must tend to infinity.…”
Section: Modifying the Usual Problemmentioning
confidence: 99%
See 1 more Smart Citation
“…It can be concluded that when the velocity v 0 is below the threshold value in equation ( 27), the sphere cannot complete the vertical loop rolling without slipping in all points of the path. Following another formulation, Tea [7] also concludes that according to the conventional solution of the classical problem (h = 2.7R), the static friction coefficient must tend to infinity.…”
Section: Modifying the Usual Problemmentioning
confidence: 99%
“…It is proved that the conventional solution found in many text books has several flaws, which are discussed and compared with the solution presented in this paper. A similar problem has already been studied in the literature [7]; however, in that work, Tea analyzes different particular cases focusing the attention around a reference initial condition h/R = 2.7, h being the initial height of the sphere and R the radius of the vertical loop, but searching for a general solution of this problem is not the focus of Tea's paper. This paper is organized as follows.…”
Section: Introductionmentioning
confidence: 99%
“…Este problema ha sido ampliamente estudiado en la literatura y se han propuesto soluciones alternativas a partir de consideraciones geométricas, utilizando los conceptos de serie de Taylor y radio de curvatura, así como las nociones de límite de una función continua y funciones trigonométricas, además de elementos de geometría euclidiana y la congruencia deángulos en triángulos isósceles [3,4]. La complejidad se incrementa cuando se considera la presencia de fricción, por ello, este problema y sus variantes pocas veces se abordan en cursos de licenciatura, sin embargo, dicho problema también ha sido ampliamente estudiado en la literatura [5][6][7][8]. A pesar de esto, el tema sigue siendo de interés desde el punto de vista teórico, experimental y educativo [9][10][11][12][13].…”
Section: Introductionunclassified
“…In a real "loop-the-loop "system, where the rolling of a solid sphere is combined with occasional sliding, relying on this equation leads to a discrepancy between the expected and experimental results [18]. As Tea Jr points out [19], in real systems, the ratio between the initial height and the loop's radius has to be at least 2.7 to ensure that the ball completes the loop.…”
Section: Introductionmentioning
confidence: 99%