We start a general form for a rightward moving wave, y(x,t)=A‌sin(kx−ωt+ϕ) ...(i) The given amplitude is A = 2 cm = 0.02 m The wavelength is given as λ=1m Wave number =k=2π∕λ=2πm−1 Angular frequency, ω=vk=10π‌rad∕s From Eq. (i), y(x,t)=(0.02)‌sin[2π(x−5t)+ϕ] ∵ For x = 0, t = 0 y=0 and
δy
δt
<0 i.e. 0.02‌sin‌ϕ=0 (as y = 0) and −0.2π‌cos‌ϕ<0 From these conditions, we may conclude that ϕ=2nπ, where n=0,2,4,6... Therefore, y(x,t)=(0.02m)‌sin[(2πm−1)x−(10πs−1)t]‌m