To solve the problem it is necessary to apply the theory of sine waves. The wavelength λ of a sinusoidal waveform traveling at constant speed v is given by
[tex]\lambda = \frac{v}{f}[/tex]
Where,
v= velocity
f = frequency
Re-arrange to find v, we have
[tex]v = f\lambda[/tex]
PART A ) Replacing with our values we have,
[tex]v = (10*10^3)(0.01)[/tex]
[tex]v = 100m/s[/tex]
PART B) In the case of the period we know that it is defined as a function of frequency as,
[tex]T= \frac{1}{f}[/tex]
That is to say that using the previously given values we have that the period in seconds is,
[tex]T=1*10^{-4}s[/tex]
PART C) Finally the transverse wave velocity is given by,
[tex]v=\sqrt{\frac{T}{\mu}}[/tex]
Where,
T= Period
[tex]\mu =[/tex] Linear mass density
Re-arrange to find [tex]\mu,[/tex]
[tex]\mu = \frac{T}{v^2}[/tex]
[tex]\mu = \frac{1*10^{-4}}{100^2}[/tex]
[tex]\mu = 1*10^{-8}kg/m[/tex]