By solving the wave equation for a string, we can find out that the velocity of a wave on it is:
[tex]v=\sqrt[\placeholder{⬚}]{\frac{T}{\frac{m}{L}}}[/tex]Where T is the tension, m is the mass and L is the length. We can calculate in our case, which leaves us with:
[tex]v=\sqrt[\placeholder{⬚}]{\frac{2000}{\frac{100}{20}}}=20\frac{m}{s}[/tex]So the velocity in which a wave propagates on this cable is 20 m/s. We can also calculate its fundamental vibration frequency, which is:
[tex]f_1=\frac{v}{2L}=\frac{20}{2*20}=0.5Hz[/tex]However, this is when there is a single "half-wave" on the cable. As we know from the exercise, the wavelength (i.e. the full wave) is 0.5m, so our cable can fit 20/0.5 or 40 full waves, which is 80 half waves.
With this in mind, we can use the formulas for a standing wave:
[tex]f=n.f_1=80*0.5=40Hz[/tex]Then, our final answer is f=40Hz