
Define the wavenumber \(k=2\pi/\lambda\), so the wave profile at \(t=0\) is \(u(x)=A\sin(kx)\).
Strain is the fractional deformation, \(\varepsilon = du/dx = Ak\cos(kx)\), whose peak value is simply \(Ak\) since \(\cos(kx)\) oscillates between \(-1\) and \(+1\).
With unit amplitude \(A=1\) and \(\lambda=16\) km,
\[k = \frac{2\pi}{16} = \frac{\pi}{8}\ \text{km}^{-1} \approx 0.3927\ \text{km}^{-1}\]
Because the amplitude is dimensionless (unit amplitude), the peak strain magnitude here equals \(k\) numerically, i.e. \(\varepsilon_{max}=\pi/8\approx 0.393\).
This can also be checked qualitatively: doubling the wavelength while keeping the same peak-to-trough displacement spreads that same displacement over twice the distance, halving the maximum strain - consistent with \(\varepsilon_{max}\propto 1/\lambda\).
\(\boxed{\varepsilon_{max}\approx 0.393}\), within the accepted band 0.385 to 0.405.