Suppose, that the frequency f depends on the tension raised to the power a, length raised to the power b and mass per unit length raised to the power c.
Then, f∝[F]a[l]b[μ]c
or, f=k[F]a[l]b[μ]c ...(i)
Here, k is a dimensionless constant.
Thus, [f]=[F]a[l]b[μ]c
or, [M0L0T−1]=[MLT−2]e[L]b[ML−1]c
or, [M0L0T−1]=[Ma+cLa+b−cT−2a]
For dimensional balance, the dimensions on both sides should be same.
Thus, a+c=0 ...(ii)
a+b−c=0 ...(iii)
−2a=−1 ...(iv)
Solving these three equations, we get
a=12,c=−12andb=−1
Substituting these values in Eq. (i), we get
f=k(F)1/2(l)−1(μ)−1/2orf=kl√Fμ
Experimentally, the value of k is found to be 12.
Hence, f=12l√Fμ