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  1. Integrator
  2. Implicit
  3. Newmark

NonviscousNewmark

PreviousWilsonPenzienNewmarkNextExplicit

Last updated 4 months ago

Newmark Time Integration With Nonviscous Damping

References

Syntax

integrator NonviscousNewmark (1) (2) (3) ((4) (5) (6) (7)...)
# (1) int, unique tag
# (2) double, alpha, typical: 0.25
# (3) double, beta, typical: 0.5
# (4) double, real part of `m_i`
# (5) double, imaginary part of `m_i`
# (6) double, real part of `s_i`
# (7) double, imaginary part of `s_i`

Theory

The parameters mim_imi​ and sis_isi​ are two complex numbers that define the kernel function.

g(t)=∑i=1nmie−sit.g(t)=\sum_{i=1}^nm_ie^{-s_it}.g(t)=i=1∑n​mi​e−si​t.

For example, if the kernel contains two exponential functions such that

g(t)=(1+9i)e−(2+8i)t+(3+7i)e−(4+6i)t,g(t)=(1+9i)e^{-(2+8i)t}+(3+7i)e^{-(4+6i)t},g(t)=(1+9i)e−(2+8i)t+(3+7i)e−(4+6i)t,

then the command shall be defined as

integrator NonviscousNewmark 1 .25 .5 1 9 2 8 3 7 4 6

It is assumed that the kernel is applied to all DoFs in the system.

As of writing, the referenced algorithm is probably the most efficient algorithm for nonviscous damping as there is no explicit integration of the convolution integral.

10.1016/j.ymssp.2024.111156