# 1 The Lorenz chaotic system

This example shows how to solve the chaotic Lorenz’ dynamical system—you know the one of the butterfly. The differential equations are

\begin{cases} \dot{x} &= \sigma \cdot (y - x)\\ \dot{y} &= x \cdot (r - z) - y\\ \dot{z} &= xy - bz\\ \end{cases}

where \sigma=10, b=8/3 and r=28 are the classical parameters that generate the butterfly as presented by Edward Lorenz back in his seminal 1963 paper Deterministic non-periodic flow.

## 1.1 lorenz.was

Please note the beauty of both the Lorenz system and the associated wasora input.

# lorenz' seminal dynamical system
PHASE_SPACE x y z
end_time = 40

# parameters
CONST sigma r b
sigma = 10
r = 28
b = 8/3

# initial conditions
x_0 = -11
y_0 = -16
z_0 = 22.5

# the dynamical system
x_dot .= sigma*(y - x)
y_dot .= x*(r - z) - y
z_dot .= x*y - b*z

PRINT t x y z HEADER

# exercise: play with the system! change
# the parameters and plot, plot plot!
$wasora lorenz.was > lorenz.dat$ qdp lorenz.dat -o lorenz2d --pt "16 17 18" --ps "0.5 0.5 0.5" --color "orange navyblue gray" --pi "60 71 87"
$gnuplot lorenz3d.gp$ 

The ability to solve the Lorenz system—that has both intrigued and inspired me since I was old enough to understand differential equations—with such simple and concise instructions shows me that indeed wasora has something to provide to the scientific/engineering community. Lorenz as a function of time The Lorenz attractor in phase space