All Solutions
Page 463: Section Review
$$theta_i=theta_r$$
Where $theta_i$ is an angle of incidence and $theta_r$ is angle of reflection, both relative to the **normal of the surface**.
This means that the angle of the reflected ray is $80^o$ relative to the normal of the surface.
$$alpha+theta_r=90^o$$
$$alpha=90^o-theta_r$$
$$alpha=90^o-80^o$$
$$boxed{alpha=10^o}$$
begin{align*}
alpha + theta_{r} &= 90 textdegree \
alpha &= 90 textdegree -theta_{r} \
alpha &= 90 textdegree – 80 textdegree \
alpha &= 10 textdegree
end{align*}
The angle betweem the reflected ray and the mirror is [ framebox[1.1width]{$ therefore alpha= 10 textdegree $}]

alpha= 10 text{textdegree}
$$
Each individual light ray of the bundle follows the law of reflection.
If the bundle of light rays is incident upon a smooth surface, then the light rays reflect and remain concentrated in a bundle upon leaving the surface.
On the other hand, if the surface is microscopically rough, the light rays will reflect and diffuse in many different directions.
The normal line at the point of incidence is different for different rays. Subsequently, when the individual rays reflect off the rough surface according to the law of reflection, they scatter in different directions.
The result is that the rays of light are incident upon the surface in a concentrated bundle and are diffused upon reflection.
text{color{#c34632}Perfectly smooth surfaces create specular reflection.
$ $
Rough surfaces create diffuse reflection.}
$$
Note that the objects which create specular reflection can act like mirrors
The following metals will create diffuse reflection :
paper, rough metal, ground glass, plastic milk jug
text{color{#c34632}For a real object, the virtual mirror will form a virtual image behind the mirror.
$ $
The size of the image will be same as that of the object
$ $
Distance of image from mirror is same as the object’s distance from mirror}
$$
It is formed 3 metres behind the mirror
Height of the Image is 50 cm

$$
begin{align*}
beta + theta_{r}&=90 text{textdegree}\
theta_{r}&=90 text{textdegree} – beta\
theta_{r}&=90 text{textdegree} – 45 text{textdegree}\
theta_{r}&=45 text{textdegree}\
end{align*}
$$
From The Law of Reflection can calculate the incident angle $theta_{i}= theta_{r} Rightarrow theta_{i}= 45 text{textdegree}$ So, we can calculate, but also we can see from the diagram, that the Sun is right above the first car. To find the position of the Sun relative to the first car, we can observe the angle between the incident angle and horizontal axis $theta_{i}+ theta_{r} = 90 text{textdegree}$

In case of diffuse reflection, the incident light is reflected in all directions.
This enables you to view the object from any angle.