-ignore the effect of thickness on lens power -central thickness is small in relation to radii
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2 curved refracting surfaces (front and back) connected together
the index of the lens is generally higher than the surrounding media
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lens power
sum of both surface powers Ft= F1 + F2
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Lens designs
convex, positive, converging, or plus lenses -thicker center, thinner edge concave, negative, diverging or minus lenses -thinner center, thicker edge opthalmic lenses: usually meniscus -minimizes off axis (peripheral) aberrations
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lenses have spherical surfaces
biconvex lens - r1 is + and F1 is + - r2 is - and F2 is + biconcave lens - r1 is - and F is - - r2 is + and F2 is -
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focal lengths
f' is image distance with the object at infinity f is the object distance with image at infinity
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refraction occurs in _____
a single plane we assume this
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focal lengths
F is the primary focal length and F' is the secondary focal length
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Thin lens imaging
-the same as for curved surfaces -F is now the power of the whole lens instead of just one side - we can assume that it has air on either side unless otherwise specified
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Thin lens imaging formula and relationship
- as RO moves from infinity to primary focal point (F), RI moves from secondary focal point (F') to infinity - if RO is inside primary focal point (F), a VI is formed - L'= L + F
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focal length formula
f=-n/F f'= n'/F
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extended objects and lateral magnification
- can examine orientation and size of image compared to the object - typically an arrow extending perpendicular to axis - point source at tip of the arrow
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Lateral magnification (LM) formula
LM= h'/h = l'/l = L/L'
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what does LM tell us
-if LM+, image is erect -if LM-, the image is inverted -if LM>1, image is larger than object (h'>h) -if LM
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lateral magnification and symmetrical planes
symmetrical planes means LM = -1 if LM =-1, the l=2 f and l'=2f'
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plus lens and distant object
- can't really find the lateral magnification because we need the image size or object size - there is a special case when an object is at infinity