Problem Analysis:
We are given the equation of a transverse wave: $y = y_0 \sin 2\pi(ft - \frac{x}{\lambda})$. We are also given the condition that the maximum particle velocity is four times the wave velocity. We need to find the relationship between the wavelength ($\lambda$) and amplitude ($y_0$).
The particle velocity ($v_p$) is the rate of change of displacement ($y$) with respect to time ($t$). We find it by differentiating the wave equation with respect to $t$:
$ v_p = \frac{\partial y}{\partial t} = \frac{\partial}{\partial t} \left[ y_0 \sin 2\pi(ft - \frac{x}{\lambda}) \right] $
Using the chain rule:
$ v_p = y_0 \cos 2\pi(ft - \frac{x}{\lambda}) \cdot \frac{\partial}{\partial t} \left[ 2\pi(ft - \frac{x}{\lambda}) \right] $
$ v_p = y_0 \cos 2\pi(ft - \frac{x}{\lambda}) \cdot (2\pi f) $
$ v_p = 2\pi f y_0 \cos 2\pi(ft - \frac{x}{\lambda}) $
The maximum value of the cosine function ($\cos \theta$) is 1. Therefore, the maximum particle velocity ($v_{p,max}$) is:
$ v_{p,max} = 2\pi f y_0 $
The wave equation can be written as $y = y_0 \sin(2\pi f t - \frac{2\pi x}{\lambda})$.
Comparing this with the standard form $y = A \sin(\omega t - kx)$, we identify:
The wave velocity ($v_w$) is given by $v_w = \frac{\omega}{k}$:
$ v_w = \frac{2\pi f}{\frac{2\pi}{\lambda}} = f \lambda $
The problem states that $v_{p,max} = 4 \cdot v_w$. Substituting the expressions we found:
$ 2\pi f y_0 = 4 \cdot (f \lambda) $
Assuming $f \neq 0$, we can cancel $f$ from both sides:
$ 2\pi y_0 = 4 \lambda $
Now, we solve for $\lambda$:
$ \lambda = \frac{2\pi y_0}{4} $
$ \lambda = \frac{\pi y_0}{2} $
The relationship derived matches Option B.
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