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Lenses, mirrors and refractive surfaces
Friday Sept. 13, 2002
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Refraction at a spherical interface: Paraxial ray approximation
Snell’s law ____________________________ Leads to… Governs refraction at an interface All rays from O pass through I, i.e. I = image of O For a given object distance s, can find a conjugate distance s’
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Definitions: Focal points of a curved interface
Governs refraction at an interface Focal Points: Suppose object at s = All rays arriving at lens will travel parallel to optic axis and, This defines the second focal point
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Definition: Focal points of a curved interface
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Definitions: Focal points of a curved interface
Suppose image at s’ = All rays leaving lens will travel parallel to optic axis and, This defines the first focal point.
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Focal points for curved interface
Show Definition: Focal points, f, f’ are conjugate with s, s’ =
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Definitions: Power n’>n Power of surface
P > 0 for converging surface C n n’ C n n’ R<0 P < 0 for diverging surface
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Definitions: Power Thus if n’ > n and R< 0 In general,
f, f’, and P are all negative In general,
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Refraction at a spherical interface
In paraxial ray approximation: Imaging occurs according to:
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Object-image height relationship
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Lateral Magnification
Since h is negative True for all imaging according to
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Lateral magnification
h R C h’ n n’ s s’ In above, since s, s’ > 0 m < 0 inverted image New image shown in figure is real (light actually passes through) inverted demagnified or reduced
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Thin lenses Treat as two spherical interfaces
Assume that the lens thickness t is negligible n n’ O I C2 C1 nL R1 R2 s s’
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Thin lens: First surface
P’ P V R1 s, R1 > 0 s s” s” < 0 since to the left of V
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Thin lens: Second surface
P’ t nL s” s’
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Thin lens: second interface
First interface Second interface Object distance t + s” = t - |s”| Thin lens t → 0, so object distance = - |s”|
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Thin lens First interface Second interface
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Thin lens In a single medium (n=n’) In air (n = 1) Lens makers formula
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Thin lens (nL=1.5): Examples
Double convex lens |R1| = |R2| = 20 cm f =____ P = _____ Double concave lens Plano-convex
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Thin lens: Power Thicker in middle P > 0 Thinner in middle P < 0
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Thin lens: Ray diagrams
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Reflection at a curved mirror interface in paraxial approx.
y φ ’ O C I s’ s
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Reflection at a curved mirror interface
Show that:
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