Answer:
(a). [tex]\dfrac{f_3'}{f_3} =\sqrt{5}.[/tex]
(b). The wavelength remains unchanged.
Explanation:
The speed [tex]v[/tex] of the waves on the string with tension [tex]T_i[/tex] is given by
[tex]v = \sqrt{\dfrac{T_iL}{m} }[/tex]
And if the string is vibrating, its fundamental wavelength is [tex]2L[/tex], and since the frequency [tex]f[/tex] is related to the wave speed and wavelength by
[tex]f = v/\lambda[/tex]
the fundamental frequency [tex]f_1[/tex] is
[tex]f_1 =\sqrt{\dfrac{T_iL}{m} }*\dfrac{1}{2L}[/tex]
and since the frequency of the third harmonic is
[tex]f_3 = 3f_1[/tex]
[tex]f_3 = 3\sqrt{\dfrac{T_iL}{m} }*\dfrac{1}{2L},[/tex]
and the wavelength is
[tex]\lambda_3 = \dfrac{2L}{3}.[/tex]
(a).
Now, if we increase to the string tension to
[tex]T_f = 5.0T_i[/tex]
the third harmonic frequency becomes
[tex]f_3' = 3\sqrt{\dfrac{5T_iL}{m} }*\dfrac{1}{2L},[/tex]
The ratio of this new frequency to the old frequency is
[tex]\dfrac{f_3'}{f_3} = \dfrac{3\sqrt{\dfrac{5T_iL}{m} }*\dfrac{1}{2L}}{3\sqrt{\dfrac{T_iL}{m} }*\dfrac{1}{2L}}[/tex]
[tex]\boxed{\dfrac{f_3'}{f_3} =\sqrt{5}.}[/tex]
(b).
The wavelength of the third harmonic remains unchanged because [tex]\lambda_3 = \dfrac{2L}{3}.[/tex] depends only on the length of the string