The speed \( v \) of a wave on a string is given by the equation \( v = (\text{constant}) F^a \left( \frac{m}{L} \right)^b \). We need to find the values of constants \( a \) and \( b \) such that this equation is dimensionally consistent.
We begin by analyzing the dimensions involved. The dimension of speed \( v \) is \([v] = [LT^{-1}]\). Given, the dimension of tension \( F \) is \([F] = [ML][T]^{-2} = [M][L][T]^{-2}\). The mass per unit length \(\frac{m}{L}\) has the dimension \([\frac{m}{L}] = [M][L]^{-1}\).
Substitute these into the equation:
\([v] = [F]^a \left[\frac{m}{L}\right]^b = ([M][L][T]^{-2})^a ([M][L]^{-1})^b\)
Solving for the dimensions, we get:
\([L][T]^{-1} = [M]^a[L]^a[T]^{-2a}[M]^b[L]^{-b}\)
Combining the dimensions, we have:
\([L][T]^{-1} = [M]^{a+b}[L]^{a-b}[T]^{-2a}\)
Set the powers of \(M\), \(L\), and \(T\) equal to each other:
From \(-2a = -1\), we get \(a = \frac{1}{2}\).
Substitute \(a = \frac{1}{2}\) into \(a + b = 0\):
\(\frac{1}{2} + b = 0 \Rightarrow b = -\frac{1}{2}\).
Checking with other relation \(a - b = 1\):
\(\frac{1}{2} - (-\frac{1}{2}) = 1\), which is correct.
Thus, the values of \(a\) and \(b\) are \(\frac{1}{2}\) and \(-\frac{1}{2}\), respectively. Hence, the correct option is:
\(a = \frac{1}{2}, b = -\frac{1}{2}\).