Consider a plane wave front travelling in vacuum incident on the surface of a block of glass at an angle of incidence i as shown in figure 9. The line XW is the section of the wavefront on the plane of the paper. Note that XW is only a portion of the wavefront (WF) moving along the incident ray SO. Due to the inclined incidence the point X reaches the surface first. Let us take this instance as t=0. As the WF enters glass, the portion of the WF in vacuum travels with speed c and the portion in glass travels with speed v which is less than c. Therefore the WF at successive instances are closer to each other in glass than in vacuum. When the point W touches the surface of glass at y, the refracted part of the section XY is represented by VY. The incident ray is along SO (perpendicular to XY), the refracted ray is along OT (perpendicular to VY). The angles of incidence and refraction are related to the speed of light as shown in the box below.