The purpose of most optical instruments is to produce an image. Images can be formed by reflection and refraction.
What is an image?
We see objects, because they either emit or reflect light. We visually identify objects by the pattern of light that they emit or reflect. We gather some portion of that light on a detector (our eyes). In interpreting the pattern, we implicitly assume that the light traveled in a straight line from the object to the detector.
Mirrors can produce real and virtual images by reflection. A flat
mirror only produces virtual images.
Light rays from the object reflect off the mirror before hitting a detector. For the detector, the apparent position of the object is behind the mirror. Let xo denote the perpendicular distance of the object from the mirror surface, and let xi denote the perpendicular distance of the image from this surface. If we let distances in front of the mirror be positive and distances behind the mirror be negative, then we have xo + xi = 0.
For mirrors, negative image distances are associated with virtual images and positive image distances are associated with real images.
For each ray θi = θr.
Multiple images can be formed by combinations of flat mirrors. In the picture to the right, light bouncing off one or both of the mirrors can reach the eye along three different paths. The detector sees three virtual images.
Determine the minimum height of a vertical, flat mirror in which a
person 5'10'' in height can see his or her full image.
The height of the mirror must be half the height of the person, in this case 2'11''.
Light rays from a distant star are nearly perfectly parallel to each other when they reach Earth. To produce a bright image of the star we want to gather as much light from the star as possible and bring it together in one spot, called a focus. A mirror with a parabolic surface can perfectly focus incoming light rays parallel to its axis. It produces a real image in the focal point of the parabola. A parabola is the locus of all points, which are equidistant from a line and a point (the focal point). All light rays from a distant source approaching the parabola parallel to its symmetry axis and reflecting from its surface have the same minimum travel time to the focal point of the parabola. By Fermat's principle light will therefore take all these paths, and the rays will come together at the focus.
A concave mirror with a spherical surface focuses light similarly to a parabolic mirror as long as the angle subtended by the spherical mirror section is small. A spherical mirror has a radius of curvature R and a focal length f = R/2. The focal length f is the distance between the focus and the surface of the mirror. The figure on the right compares a parabolic and a concave spherical surface with the same focal length f. Near the symmetry axis or optical axis the curves are nearly identical.
As long as all light rays stay close to and make small angles with the optical axis,
we can write down a simple formula for spherical mirrors relating object and
image distances and the radius of curvature and focal length. This formula
is valid in the paraxial approximation.
If an object is placed in front of a spherical mirror at an object distance xo, then an image is formed at an image distance xi, where xo and xi satisfy the mirror equation,
1/xo + 1/xi = 1/f = 2/R.
Sign conventions for the mirror equation:
xi is positive for a real image in front of the mirror surface, and xi is negative
for a virtual image behind the mirror surface.
xo and xi are the perpendicular distances from the center plane of the mirror as shown in the drawing below.
The focal length f and the radius of curvature R = 2f are positive for a concave mirror and negative for a convex mirror. For a concave mirror the reflecting surface bulges inward, and for a convex mirror the reflecting surface bulges outward.
We can also determine the positions and sizes of images of points formed by spherical mirrors geometrically by drawing ray diagrams. Only two rays must be drawn.
Rules for drawing ray diagrams:
In the example diagram a real image is formed by a concave mirror.
The image, in general, has not the same size of the object.
We define the magnification M as the ratio of the height of the image hi to the height of the object ho. We have from geometry
M = hi/ho= -xi /xo .
If the magnification is negative, the image is inverted.
Here are some things that always go together for curved mirrors.
Convex mirrors form only virtual images.
Concave mirrors form real images, if xo > f and virtual images if xo < f. The type of image formed depends on the position of the object.
A concave mirror has a radius of curvature of 20 cm. Find the location
of the image for object distances
(a) 40 cm, (b) 20 cm, (d) 10 cm.
For each case state whether the image is real or virtual, and upright or inverted. Find the magnification for each case.
Mirror equation: 1/xo + 1/xi = 1/f.
For a concave mirror f is positive. f = R/2. For this mirror f = 10 cm.
(a) 1/10 - 1/40 = 1/xi. 3/40 = 1/xi. xi = 13.33 cm. The image is real.
M = -xi/xo = -1/3. The image is inverted.
b) 1/10 - ½0 = 1/xi. ½0 = 1/xi. xi = 20 cm. The image is real.
M = -xi/xo = -1. The image is inverted.
(c) 1/10 - 1/10 = 1/xi. 0 = 1/xi. There is no finite image distance. All rays from the object are parallel after reflection.
A object 2 cm in height is placed 3 cm in front of a concave mirror. If
the image is 5 cm in height and virtual, what is the focal length of the
M = -xi/xo = 5/2. xo = 3 cm, therefore xi = -7.5 cm.
1/xo + 1/x i= 1/f. 1/3 - 1/7.5 = 1/f. f = 5 cm.
If an object placed 10 cm in front of a convex mirror produces a virtual
image 5 cm behind the mirror, what is the focal length of the mirror?
1/10 - 1/5 = 1/f. f = -10 cm.
A concave mirror forms an inverted image, four times larger than the object.
If the distance between image and object is 1.5 m, find the radius of curvature
R of the mirror.
An inverted image is a real image. It forms in front of the mirror, the image distance is positive.
We have M = -xi/xo = -4, xi = 4xo.
(1/xo) + 1/(4xo) = 1/f, f = (4/5)xo.
xo is not given, but the distance between xi an xo is given.
xi = 4xo, and both object and image are in front of the mirror.
Therefore the distance between image and object = 4xo - xo = 3xo = 1.5 m.
xo = 0.5 m, f = (4/5)xo = 0.4 m.
R = 2f = 0.8 m.
Additional information: The Physics Classroom: Reflection and the Ray Model of Light