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Fiabilitate si Durabilitate - Fiability & Durability Supplement no 1/ 2012

Editura “Academica Brâncuşi” , Târgu Jiu, ISSN 1844 – 640X 68

DETERMINING THE RESPONSE IN CASE OF VIBRATIONS OF

STRAIGHT BARS WITH RANDOM EXCITATIONS

Ph.D.Lecturer Monica BALDEA,Faculty of Mechanics and Technology,University of Pitesti,e-mail:bldmonica@yahoo.com

Abstract:By applying the finite element calculus to the study of bar vibrations, one obtains a system of linear

diferential equations. One carries out the determination of the response to random stimulations by calculating the statistical terms as a function of the statistical terms of the stimulation.

Key words:random,vibrations, bar, response.

1.Introduction

The exact mathematical model of the bars vibrations leads, as we know, at solving some partial derivative equations.

The difficulties we come across solving this equations start from the limit conditions as well from the stimulation that solicits the bars.

Paper [5] shows that the difficulties concerning the limit conditions can be avoid by using the finite element calculus. The paper which we present shows that by applying the finite element calculus we can avoid the difficulties concerning stimulations too, especially the random ones, in which the response must be expressed in stimulation statistic terms.

2.Differential equation of the finite element (the finite elements differential equations) Let s take a straight bar constant section, with area A and length L and AiAj the finite element with length l noted with index p.

We will note OXYZ the reference system, and Ai xyz the local reference system, and Ai xyz the local reference system.

During the following equations we will study only the bars plane vibrations. We will use for the knots Ai Aj displace in the local reference system, the notes

(1) And for the knots Ai Aj faces the notes

(2) If m is the finite elements mass, E the longitudinal elasticity module I the inertia moment from the normal sections Aiz axis, than based on the notes from paper [5]

(3)

We obtain the inertia matrix

(2)

Fiabilitate si Durabilitate - Fiability & Durability Supplement no 1/ 2012

Editura “Academica Brâncuşi” , Târgu Jiu, ISSN 1844 – 640X 69

(5)

and the rigidity matrix: (6)

(7)

The differential equations of the finite elements vibrations, in the local reference system are the same in this case with the differential equations from the general system (8)

3.Equations assembly If in the Ai knots the external forces Pi operates (acts) and the use notes (9)

Taking into account the equality For the knot Ai we obtain the equation (10)

The relations written for all the non-zero displacement knots can be written in one matrix equation (11)

Where M is the bars inertia matrix K is the bars rigidity matrix is the displacement vector and P the stimulations vector So for the bar embedded at the ends from considering only three finite elements (12)

(13)

(14)

; (15)

(3)

Fiabilitate si Durabilitate - Fiability & Durability Supplement no 1/ 2012

Editura “Academica Brâncuşi” , Târgu Jiu, ISSN 1844 – 640X 70

(17)

(18)

(19)

(20)

Considering the first and fourth scalar equation resulting from the (11) equation, we obtain the system (21)

Result in system (21) beats value: (22)

Which is very similar to the exact value[6] 4.The response to random stimulation Lets further consider that stimulation{P}from the (11) equation is a stationary random vector function and ergodic and lets determin the responses terms. We calculate the transfer matrix (23)

and considering that the interspectral density matrix of power is know, results[ 4]: -mean value vector (24)

-interspectral density matrix (25)

(4)

Fiabilitate si Durabilitate - Fiability & Durability Supplement no 1/ 2012

Editura “Academica Brâncuşi” , Târgu Jiu, ISSN 1844 – 640X 71

Bibliography

[1] Buzdugan Gh. ,Fetcu L., Rades M., Vibrations of mechanical systems, Bucharest Academy Publishing House,1975

[2] Cuteanu E., Marinev R., Finite element method in design of structures,Facla Publishing House,Bucharest,1980

[3]Marinescu G.,Ivan C., Finite Element Method, C.I.A.Publishing House,Bucuresti,1996 [4]Munteanu M.,Introduction in the dynamics of solid rigid oscillations and of solid rigid

systems,ColoseumPublishing House, Cluj Napoca,1977

[5]Pandrea N.,Rizea V., Finite Element Method. Concepts and aplications, Publisher University of Pitesti,1998

[6]Pandrea N., Parlac S.,Mechanical vibrations ,Publisher University of Pitesti,2000

Referências

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