newmark.RdNewmark's is a method to solve higher-order differential equations without passing through the equivalent first-order system. It generalizes the so-called `leap-frog' method. Here it is restricted to second-order equations.
newmark(f, t0, t1, y0, ..., N = 100, zeta = 0.25, theta = 0.5)function in the differential equation \(y'' = f(x, y, y')\);
defined as a function \(R \times R^2 \rightarrow R\).
start and end points of the interval.
starting values as row or column vector;
y0 needs to be a vector of length 2, the first component
representing y(t0), the second dy/dt(t0).
number of steps.
two non-negative real numbers.
Additional parameters to be passed to the function.
Solves second order differential equations using the Newmark method
on an equispaced grid of N steps.
Function f must return a vector, whose elements hold the evaluation
of f(t,y), of the same dimension as y0. Each row in the
solution array Y corresponds to a time returned in t.
The method is `implicit' unless zeta=theta=0, second order if
theta=1/2 and first order accurate if theta!=1/2.
theta>=1/2 ensures stability.
The condition set theta=1/2; zeta=1/4 (the defaults) is a popular
approach that is unconditionally stable, but introduces oscillatory
spurious solutions on long time intervals.
(For these simulations it is preferable to use theta>1/2 and
zeta>(theta+1/2)^(1/2).)
No attempt is made to catch any errors in the root finding functions.
List with components t for grid (or `time') points between t0
and t1, and y an n-by-2 matrix with solution variables in
columns, i.e. each row contains one time stamp.
Quarteroni, A., R. Sacco, and F. Saleri (2007). Numerical Mathematics. Second Edition, Springer-Verlag, Berlin Heidelberg.
This is for demonstration purposes only; for real problems or applications
please use ode23 or rk4sys.
# Mathematical pendulum m l y'' + m g sin(y) = 0
pendel <- function(t, y) -sin(y[1])
sol <- newmark(pendel, 0, 4*pi, c(pi/4, 0))
if (FALSE) { # \dontrun{
plot(sol$t, sol$y[, 1], type="l", col="blue",
xlab="Time", ylab="Elongation/Speed", main="Mathematical Pendulum")
lines(sol$t, sol$y[, 2], col="darkgreen")
grid()} # }