A linearly polarised electromagnetic wave given as E=E0i^cos(kz-ωt) is incident normally on a perfectly reflecting infinite wall at z = a. Assuming that the material of the wall is optically inactive, the reflected wave will be given as:

1. Er=-E0i^cos(kz-ωt)

2. Er=E0i^cos(kz+ωt)

3. Er=-E0i^cos(kz+ωt)

4. Er=E0i^sin(kz-ωt)