In the lowest order, the velocity of transverse waves in a chain freely hanging may be given by

where x is the distance from the lower, free end of the chain. The wave velocity is strongly dependent on the location and the chain can be regarded as a typical nonuniform wave medium. The differential equation to describe transverse waves in the chain is given by (See Note No. 8 for detailed derivation.) This is not in the form of standard wave equation. For a narrow pulse, the term of first order derivative can be ignored, which yields the approximated propagation velocity given in the first equation.Standing wave in the form

satisfies This can be satisfied by the zero-th order Bessel function where L is the length of he chain. At the upper end**Standing waves in a chain vertically hung (typical
nonuniform wave medium).**

**Lowest order mode.**

`> `**with(plots):**
**animate([.1*BesselJ(0,2.4048*sqrt(x))*sin(t),x,x=0..1],t=0..2*Pi,frames=60,color=red);**

**Second mode.**

`> `**animate([BesselJ(0,5.5201*sqrt(x))*sin(1.81*t),x,x=0..1],t=0..2*Pi/1.81,frames=30,color=red);**

**Third mode.**

`> `**animate([BesselJ(0,8.6537*sqrt(x))*sin(3.6*t),x,x=0..1],t=0..2*Pi/3.6,frames=20,color=red);**

`>`