sdof problem

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Structural Engineering Program CEE 536—Structural Dynamics Instructor: Keith D. Hjelmstad Spring 2014 Homework Problems Homework 6 The single degree of freedom system shown at right has a nonlinear restoring force r(u) and it subjected to an applied force f(t). The equations of motion (and initial conditions) are Un-damped System 0 () ( ( )) () (0) (0) o mu t rut ft u u u v + = = = Consider the nonlinear response function to be elasto-plasticity with stiffness k and limiting force σ o (symmetric in tension and compression). Newmark’s method satisfies the equation of motion at the discrete time points and approximates the velocity and displacement with approximations to integrals. Hence, the discrete equations are () ru m () ut SDOF corp 1 1 1 1 2 1 1 1 2 ( ) 0 (1 ) ( ) n n n n n n n n ma ru v c h a u b h a γ β + + + + + + + = = + = + Implement Newmark’s method, including a Newton loop to solve the nonlinear equations of motion for elasto-plastic model. Explore the response of the system and the influence of nonlinearity relative to the linear elastic response. () ft 2 n n n n n n n c v h a b u hv h a γ β = + = + + 1 2 () sin ft F F t = + Consider also the specific loading function where F 1 and F 2 , and are constants that describe the forcing function (i.e., a constant part and a sinusoidally varying part. () ru u k k k o σ o σ

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Single degree of freedom problem.

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  • Structural Engineering Program CEE 536Structural DynamicsInstructor: Keith D. Hjelmstad

    Spring 2014 Homework Problems

    Homework 6

    The single degree of freedom system shown at right has anonlinear restoring force r(u) and it subjected to an appliedforce f(t). The equations of motion (and initial conditions) are

    Un-damped System0

    ( ) ( ( )) ( )(0)(0)

    o

    mu t r u t f tu uu v

    + ==

    =

    Consider the nonlinear response function to beelasto-plasticity with stiffness k and limiting forceo (symmetric in tension and compression).

    Newmarks method satisfies the equation of motion at the discrete time points and approximates thevelocity and displacement with approximations to integrals. Hence, the discrete equations are

    ( )r um

    ( )u t

    SDOFcorp

    1 1

    1 12 1

    1 12

    ( ) 0(1 )( )

    n n

    n n n

    n n n

    ma r uv c h au b h a

    + +

    + +

    + +

    + =

    = +

    = +

    Implement Newmarks method, including a Newton loop to solve the nonlinear equations of motion forelasto-plastic model. Explore the response of the system and the influence of nonlinearity relative to thelinear elastic response.

    ( )f t

    2n n n

    n n n n

    c v h ab u hv h a

    = +

    = + +

    1 2( ) sinf t F F t= +

    Consider also the specific loading function

    where F1 and F2, and are constants that describethe forcing function (i.e., a constant part and asinusoidally varying part.

    ( )r u

    u

    k kk

    o

    o

    Slide Number 1