Jellyfish locomotion Jellyfish move by contracting an elastic part of their
body, called a bell, that creates a high-pressure jet of water. When the
contractive force stops, the bell then springs back to its natural shape.
Jellyfish locomotion has been modeled using a second-order linear differential
equation having the form
\(m x^{\prime \prime}(t)+b x^{\prime}(t)+k x(t)=0\)
where \(x(t)\) is the displacement of the bell at time \(t, m\) is the mass of the
bell (in grams), \(b\) is a measure of the friction between the bell and the
water (in units of \(N / m \cdot s ),\) and \(k\) is a measure of the stiffness of
the bell (in units of \(N / m )\) Suppose that \(m=100 \mathrm{g}, b=0.1
\mathrm{N} / \mathrm{m} \cdot \mathrm{s},\) and \(k=1 \mathrm{N} / \mathrm{m}\)
(a) Define the new variables \(z_{1}(t)=x(t)\) and \(z_{2}(t)=x^{\prime}(t),\) and
show that the model can be expressed as a system of two first-order linear
differential equations.
(b) Construct the phase plane, including the nullclines, for the equations
from part (a).