Summary
An elastically supported beam of infinite length, initially at rest, carries a variable concentrated force\(\overline K (\overline t )\) at a prescribed point A. General expressions are given for the deflection and the bending moment at A (6.3 and 6.4). Three special cases are considered; the first one is defined by\(\overline K (\overline t )\)=0 for\(\overline t \) and\(\overline K (\overline t )\)=K=const. for\(\overline t \); the second one by\(\overline K (\overline t )\)=0 for 0 >\(\overline t \)>\(\overline t _s \),\(\overline K (\overline t )\) given function of\(\overline t \) for 0⩽\(\overline t \)⩽\(\overline t _s \); the third one applies to problems in which, during the period of impact,\(\overline K (\overline t )\) itself is an unknown. The results given here may be of use in those railway-engineering problems in which a rail can be considered as a beam of infinite length, and in which the supporting ground has the required properties.
Similar content being viewed by others
Author information
Authors and Affiliations
Rights and permissions
About this article
Cite this article
Esmeijer, W.L. On the dynamic behaviour of an elastically supported beam of infinite length, loaded by a concentrated force. Appl. Sci. Res. 1, 151–168 (1949). https://doi.org/10.1007/BF02120325
Received:
Published:
Issue Date:
DOI: https://doi.org/10.1007/BF02120325