This is called the mirror equation
Slide 8
Image Formed by a Concave Mirror
Slide 9
If an object is very far away, then p = and 1/p = 0
Incoming rays are essentially parallel
In this special case, the image point is called the focal point
The distance from the mirror to the focal point (f) is called the focal length
The focal point is dependent solely on the curvature of the mirror, not by the location of the object
Slide 10
A convex mirror is sometimes called a diverging mirror
The rays from any point on the object diverge after reflection as though they were coming from some point behind the mirror
The image is virtual because it lies behind the mirror at the point where the reflected rays appear to originate
In general, the image formed by a convex mirror is upright, virtual, and smaller than the object
Slide 11
Image Formed by a Convex Mirror
Slide 12
Sign Conventions for Mirrors
Slide 13
Ray diagrams can be used to determine the position and size of an image
They are graphical constructions which tell the overall nature of the image
They can be used to check the parameters calculated from the mirror and magnification equations
To make the ray diagram, one needs to know the position of the object and the position of the center of curvature
Three rays are drawn; they all start from the same position on the object
Slide 14
Ray Diagrams
The intersection of any two of the rays at a point locates the image
The third ray serves as a check of the construction
Ray 1 is drawn parallel to the principal axis and is reflected back through the focal point, F
Ray 2 is drawn through the focal point and is reflected parallel to the principal axis
Ray 3 is drawn through the center of curvature and is reflected back on itself
Slide 15
Ray Diagrams
The rays actually go in all directions from the object
The three rays were chosen for their ease of construction
The image point obtained by the ray diagram must agree with the value of q calculated from the mirror equation
Slide 16