Using E=E0−ei(kz−ωt) Given, at t=t1,z=z1,E=0 the next zero that occurs in it's neighborhood is at z2, the frequency of the electromagnetic wave at t2 ei(kz1−ωt1)=ei(kz2−ωt2)kz1−ωt1=kz2−ωt2(t2−t1)ω=k(z−z1) where k=λ2π=2πv(t2−t1)=λ×2πv2π(z2−z1) =x×v1(z2−z1)⇒λ×v=(t2−t1)(z2−z1)=C(t2−t1)=C(z2−z1) Frequency is f∝t1 then (t2−t1)1=(z2−z1)C∴ Frequency, f=(z2−z1)3×108