1 edition of **Higher mode dynamic plastic response of beams with finite-deflections** found in the catalog.

- 5 Want to read
- 19 Currently reading

Published
**1976**
by Available from National Technical Information Service in Springfield, Va
.

Written in English

- Civil engineering

The Physical Object | |
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Pagination | 1 v. ; |

ID Numbers | |

Open Library | OL25411836M |

A 'read' is counted each time someone views a publication summary (such as the title, abstract, and list of authors), clicks on a figure, or views or downloads the full-text. In this paper, dynamic response of an infinitely long beam resting on a foundation of finite depth, under a moving force is studied. The effect of foundation inertia is included in the analysis by modelling the foundation as a series of closely spaced axially vibrating rods of finite depth, fixed at the bottom and connected to the beam at the top.

ABSTRACT OF THE THESIS A Study of Large Deﬂection of Beams and Plates by Vinesh V. Nishawala Thesis Director: Dr. Haim Baruh For a thin plate or beam, . Elastic -plastic beam bending y For M>Me the beam is in the elastic-plastic regime: the core of the beam (between y=- c and y=c) is in the elastic regime, while the outer fibers are in the plastic regime (σ=σy). εxx = -y/ρ y σxx σy for rectangular beams: Mp = (σy BH) / 4 = Me 2 ε σ σy εy = σy/E elastic-perfectly plastic.

American Institute of Aeronautics and Astronautics Sunrise Valley Drive, Suite Reston, VA Same as free-free beam except there is no rigid-body mode for the fixed-fixed beam. Fixed - Pinned f 1 = U» ¼ º «¬ ª S EI L 2 1 2 where E is the modulus of elasticity I is the area moment of inertia L is the length U is the mass density (mass/length) P is the applied force Note that the free-free and fixed-fixed have the same.

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On the other hand, the stationary plastic bending hinge formed at the root of the beam lasts a relatively longer time in Phase-3, and thus, it is an important response mode in the dynamic response of the cantilever beam studied in the present paper.

Download: Download high-res image (KB) Download: Download full-size image; Fig. 14 Cited by: 9. Higher mode dynamic plastic response of beams with finite. Higher mode dynamic plastic response of beams with finite-deflections. By Carlos AntGonio Pancada Guedes Soares Get PDF (6 MB)Author: Carlos AntGonio Pancada Guedes Soares.

Dynamic equilibrium of a simply supported beam. Dynamic elasto-plastic response of beams where Y(t), Y(t) = deflection and acceleration at beam midspan, respectively; 8, ~ = angular rotation and acceleration at beam support, respect- ively; I0 = mass moment of inertia with respect to point 0: I0 = / r2dm = p (Ix + Iy).Cited by: 5.

The concept of Saturation Impulse is put forward for the dynamic response of rigid, perfectly plastic structures with finite deflections subjected to rectangular pressure pulse. The value of dimensionless saturation impulse for both simply supported and fully clamped beams are by: An analytical procedure, which retains the influence of finite deflections, is developed herein for the dynamic behaviour of rectangular shaped rigid-plastic beams.

In the general formulation of the problem deformation is assumed to proceed under two distinct mechanisms depending on the extent to which the value of the peak pressure exceeds the static collapse pressure of the beam. These. A frame member is assumed to be the assemblage of an elastic beam-column and two plastic hinges at the ends of the member.

Each plastic hinge presents plastic softening behavior under bending and. An approximate theoretical procedure is developed herein in order to estimate the permanent transverse deflections of beams and arbitrarily shaped plates which are subjected to large dynamic.

To check this condition, one needs to work out A simple method for first dynamic mode of plastic deformation the axial force at A, which involves the computation of acceleration first. When F is sufficiently large, a second hinge occurs at H which leads to the second mode of deformation.

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Issue 6 (June ). Euler–Bernoulli beam theory (also known as engineer's beam theory or classical beam theory) is a simplification of the linear theory of elasticity which provides a means of calculating the load-carrying and deflection characteristics of covers the case for small deflections of a beam that are subjected to lateral loads only.

It is thus a special case of Timoshenko beam theory. Dynamic Analysis of Fixed-Fixed Beams A THESIS SUBMITTED IN PARTIAL FULFILMENT OF THE REQUIREMENT FOR THE DEGREE OF Master of Technology in Natural Frequencies and Mode Shapes 27 Evaluation of Eigenvalues and.

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It is an attempt to respond to some of. Chapter 2. Design of Beams – Flexure and Shear Section force-deformation response & Plastic Moment (Mp) • A beam is a structural member that is subjected primarily to transverse loads and negligible axial loads.

• The transverse loads cause internal shear forces and bending moments in the beams as shown in Figure 1 below. w P V(x) M(x.Dynamic flexure of rigid-plastic beams under the action of a concentrated load Yu.

R. Lepik Soviet Applied Mechanics vol pages – () Cite this article.The resistance of sandwich beams to dynamic loads remains to be fully investigated in order to quantify the advantages of sandwich construction over monolithic designs for application in shock resistant structures.

The response of the monolithic beams to shock type dynamic loadings has been investigated extensively over the past ﬁfty years or so.