To solve the given problem, we need to analyze each option in terms of dimensional analysis. Dimensional analysis is a process that checks the consistency of equations by comparing the dimensions on both sides.
The equation of the stationary wave mentioned is:
\(y = 2A \sin\left(\frac{2\pi}{\lambda} \cdot nt\right) \cos\left(\frac{2\pi}{\lambda} \cdot x\right)\)
Let's analyze each option:
- Dimension of \(x\) is [L]:
- In the term \(\cos\left(\frac{2\pi}{\lambda} \cdot x\right)\), the argument of a cosine function is dimensionless.
- This implies that \(x\) divided by \(\lambda\) (a length) is dimensionless, i.e., \([\frac{x}{\lambda}] = [1]\).
- Thus, the dimension of \(x\) is indeed [L].
- Dimension of \(n\) is [LT-1]:
- In the term \(\sin\left(\frac{2\pi}{\lambda} \cdot nt \right)\), for the argument to be dimensionless, \(\frac{nt}{\lambda}\) should be dimensionless.
- Thus, \([nt] = [L]\), where \(\lambda\) has a dimension [L]. Hence, \([n] = [L][T^{-1}]\).
- Dimension of \(\frac{n}{\lambda}\) is [T]:
- The dimension of \(n\) is found to be [LT-1].
- The dimension of \(\lambda\) is [L].
- Thus, \(\frac{n}{\lambda} = \frac{[L T^{-1}]}{[L]} = [T^{-1}]\), not [T].
- Therefore, this option is incorrect according to dimensional analysis.
- Dimension of \(nt\) is [L]:
- As detailed in option 2, for the argument to be dimensionless: \(\frac{nt}{\lambda} = 1\).
- This implies that \([nt] = [L]\), as \(\lambda\) is [L].
Based on this analysis, the incorrect statement with respect to dimensions is:
The dimension of \(\frac{n}{\lambda}\) is [T].