No, you wouldn't be able to.
REFLECTION: IF a light ray in incident on a surface if it bring back to same medium is called reflection REFRACTION: IF a light ray in incident on a surface and going to another medium is called reflection and there is a a law for refraction that is SNELL'S LAW
The substance's index of refraction isSpeed of light in vacuum / Speed of light in the substance
When a ray of light from a medium is incident on another medium with different optical density, the ray bends due to refraction. The perpendicular distance between the emergent ray and the incident ray is called the lateral shift. The angle which the incident ray makes with the normal is called angle of incidence denoted by 'i' and the angle made by the refracted ray with the normal is called the angle of refraction denoted by 'r'. Lateral shift is given by the formula:- Where t is the thickness of the glass slab, i is the angle of incidence and r is the angle of refraction
This is total internal reflection where the angle of refraction is 90 degrees and its incident angle would be the critical angle(angle of incident for which the angle of refraction is 90).... This hapens when the angle of incidence is in a medium more dense than the angle of refraction's medium
As it is parallel to the normal to the surface, the angle of incidence is zero and hence the angle of refraction also has to be zero. Hence no deviation and no refraction.
Rays at normal incidence ... perpendicular to the interface ... obey the same law of refraction that rays at any other angle do. I won't write the equation of refraction here, because you probably already know what it looks like, and if you're a little rusty, you can easily find it on line or in your Physics text as "Snell's Law". The law of refraction relates the angles with respect to the normal in each medium to the index of refraction in each medium. In the formula, the angles are referenced in terms of their sines. If the incident ray is perpendicular to the interface, then the sine of the angle of incidence is zero. Then, regardless of the relative optical densities of the two media, the sine of the angle of refraction is also zero. The ray that arrives along the normal is refracted after all, through an angle of zero.
Reflection happens only at the interface between two media, and two media with the same index of refraction act as if they were a single medium. Thus, at the interface between media with the same index of refraction, there is no reflection, and the ray keeps going straight. Continuing this line of thought, it is not surprising that we observe very little reflection at an interface between media with similar indices of refraction.
A refracted ray passes through the medium, at a different angle to the normal than the incident ray. by Ronan Lavery
c divided by the index of refraction of the medium = the speed of light in the medium.
Total internal reflection can happen only when a beam of light travelling through a dense medium crosses the interface with a rarer medium. For example, through a glass piece to air. When such a beam reaches an interface it makes an angle (called the angle of incidence) with the perpendicular at that point. When the beam exits the interface into the rarer medium. it makes a larger angle(called the angle of refraction) with the same perpendicular. As the angle of incidence increases, so does the angle of refraction. There is one value of the angle of incidence for which the angle of refraction is 90 degrees and the emerging ray is tangential to the interface. This is called the critical angle. For all angles of incidence greater than the critical angle the incident ray will not emerge into the rarer medium at all. In stead it gets reflected back into the denser medium itself. This phenomenon is called total internal reflection. Rainbows are a result of this phenomenon.
Total internal reflection can happen only when a beam of light travelling through a dense medium crosses the interface with a rarer medium. For example, through a glass piece to air. When such a beam reaches an interface it makes an angle (called the angle of incidence) with the perpendicular at that point. When the beam exits the interface into the rarer medium. it makes a larger angle(called the angle of refraction) with the same perpendicular. As the angle of incidence increases, so does the angle of refraction. There is one value of the angle of incidence for which the angle of refraction is 90 degrees and the emerging ray is tangential to the interface. This is called the critical angle. For all angles of incidence greater than the critical angle the incident ray will not emerge into the rarer medium at all. In stead it gets reflected back into the denser medium itself. This phenomenon is called total internal reflection. Rainbows are a result of this phenomenon.
-- Its speed becomes less in the denser medium. -- Its wavelength becomes greater in the denser medium. -- If its direction is not perpendicular to the boundary between the media, then its path in the denser medium is closer to the perpendicular. (This is 'refraction'.)