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Concave Mirrors

 

basic diagram

ray diagrams

proof of r = 2f

mirror formula

caustic curves

parabolic mirrors

 

 

 

Basic Ray Diagram

 

 

basic ray diagram for a concave mirror

 

 

The basic ray diagram for a concave mirror introduces a number of important terms:

 

 

aperture - the diameter of the circular mirror

 

pole - where the principal axis meets the mirror surface

 

centre of curvature - the centre of the sphere that the mirror forms part

 

radius of curvature (r) - radius of the sphere

 

principal axis - the line through the centre of curvature and the pole of the mirror

 

focal length (f) - equal to half the radius of curvature f = r/2

 

 

 

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Ray Diagrams

 

Ray diagrams are constructed by taking the path of three distinct rays from a point on the object:

 

 

X) a ray parallel to the principal axis reflected through F (the principal focus)

 

Y) a ray passing through C which is then reflected back along its original path

 

Z) a ray passing through F, which is then reflected parallel to the principal axis

 

 

note - the concave mirror is considered to be so thin as to be represented by a vertical line

 

 

construction rays for a concave mirror

 

 

The image types and positions for a concave mirror are very similar to those of a convex lens.

 

 

object between F and the mirror

This is similar to a magnifying glass, with a practical use as a make-up mirror.

 

object at F

The image is formed at infinity from parallel rays that do not converge. Therefore no image is formed.

 

object between F and C

The image is real, inverted and magnified.

 

object at C

The image is formed at C.
The image is inverted, real and the same size as the object.

 

object at infinity

The image is formed at the focal point of the lens. It is real, inverted and diminished in size.

 

 

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Proof of r = 2f

 

 

proof of r equals 2f for a concave mirror

 

 

The angle of incidence equals the angle at C (corresponding angles).

 

From the diagram it is apparent that XF does not equal PF. However, when point X is closer to the principal axis, XF approaches the size of PF.

 

So for rays close to the principal axis we can say that XF = PF.

 

In other words,

XC = PF + FC

 

r = f + f

 

r = 2f

 

 

 

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The Mirror Formula

 

 

concave mirror formula derivation

 

 

The sign convention, 'real is positive' is used:

 

 

1) focal length (f) and radius of curvature (r) are both positive for concave mirrors

 

2) distances to real images and real objects are positive

 

3) distances to virtual images and virtual objects are negative

 

 

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Caustic Curves

 

 

caustic curve of a concave mirror

 

 

The caustic is the name given to the region of a concave mirror where parallel rays of light come to different foci.

 

This happens for rays away from the principal axis. The further away they are, the closer is the focus to the mirror.

 

 

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Parabolic Mirrors

 

 

ray diagram for a parabolic mirror

 

 

A parabolic mirror produces one focus for all rays parallel to the principal axis, irrespective of their distance from it.

 

Parabolic mirrors have uses in telescopes, solar furnaces, and car headlights/torches/floodlights etc.

 

 

 

 

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