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Lecture 25 Lecture 25 Physics 2102 Jonathan Dowling Optics: Images Optics: Images

Lecture 25 - phys.lsu.eduphys.lsu.edu/~jdowling/PHYS21024SP07/lectures/lecture25.pdf · Lecture 25 Physics 2102 Jonathan Dowling Optics: Images. Thin Lenses pif 111 += For small angles

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Page 1: Lecture 25 - phys.lsu.eduphys.lsu.edu/~jdowling/PHYS21024SP07/lectures/lecture25.pdf · Lecture 25 Physics 2102 Jonathan Dowling Optics: Images. Thin Lenses pif 111 += For small angles

Lecture 25Lecture 25

Physics 2102Jonathan Dowling

Optics: ImagesOptics: Images

Page 2: Lecture 25 - phys.lsu.eduphys.lsu.edu/~jdowling/PHYS21024SP07/lectures/lecture25.pdf · Lecture 25 Physics 2102 Jonathan Dowling Optics: Images. Thin Lenses pif 111 += For small angles

Thin LensesThin Lenses

fip

111=+

For small angles and thin lenses,

Convergent: f positive

Divergent: f negative

!"

#$%

&''=21

11)1(

1

rrn

fLens maker’s equation

Convergent lens

Divergent lens

Page 3: Lecture 25 - phys.lsu.eduphys.lsu.edu/~jdowling/PHYS21024SP07/lectures/lecture25.pdf · Lecture 25 Physics 2102 Jonathan Dowling Optics: Images. Thin Lenses pif 111 += For small angles

Images due to lenses:

• An object placed beyond a convergent lenses’ focal point, will produce a real, inverted image on the other side of the lens. This is the principle used in projectors.

• An object placed between a convergent lens and its focal point will produce a virtual image on the same side as the object.

•Divergent lenses always produce a virtual image on the same side asthe object.

• Real images have i positive in formulas, virtual images have i negative.

Page 4: Lecture 25 - phys.lsu.eduphys.lsu.edu/~jdowling/PHYS21024SP07/lectures/lecture25.pdf · Lecture 25 Physics 2102 Jonathan Dowling Optics: Images. Thin Lenses pif 111 += For small angles

Locating images by drawing rays:

• A ray of direction initially parallel to the axis will pass through the focal point.

• A ray that initially has a direction thatpasses through the focal point will emerge parallel to the central axis.

• A ray going through the center of thelens will be undeflected.

• The image of a point appears where all rays emanating from a point intersect.

Page 5: Lecture 25 - phys.lsu.eduphys.lsu.edu/~jdowling/PHYS21024SP07/lectures/lecture25.pdf · Lecture 25 Physics 2102 Jonathan Dowling Optics: Images. Thin Lenses pif 111 += For small angles

ExampleExample• An object 1.2cm high is placed 4cm from a bi-convex lens withr1=10cm and r2=15cm. Find the position and size of the image.

• A second lens of focal length +6cm is placed 12cm to the right ofthe first lens. Find the position and size of the new image.

Page 6: Lecture 25 - phys.lsu.eduphys.lsu.edu/~jdowling/PHYS21024SP07/lectures/lecture25.pdf · Lecture 25 Physics 2102 Jonathan Dowling Optics: Images. Thin Lenses pif 111 += For small angles

Images fromImages fromspherical mirrorsspherical mirrors

fip

111=+

Consider an object placed between the focalpoint and the mirror. It will produce a virtualimage behind the mirror.

When the object is at the focal point theimage is produced at infinity.

If the object is beyond the focal point, a realimage forms at a distance i from the mirror.

Check the signs!!

p

im !=

lateralmagnification

Page 7: Lecture 25 - phys.lsu.eduphys.lsu.edu/~jdowling/PHYS21024SP07/lectures/lecture25.pdf · Lecture 25 Physics 2102 Jonathan Dowling Optics: Images. Thin Lenses pif 111 += For small angles

Thin LensesThin Lenses

fip

111=+

For small angles and thin lenses,

Convergent: f positive

Divergent: f negative

!"

#$%

&''=21

11)1(

1

rrn

fLens maker’s equation

Convergent lens

Divergent lens

Page 8: Lecture 25 - phys.lsu.eduphys.lsu.edu/~jdowling/PHYS21024SP07/lectures/lecture25.pdf · Lecture 25 Physics 2102 Jonathan Dowling Optics: Images. Thin Lenses pif 111 += For small angles

Locating images by drawing rays:

• A ray of direction initially parallel to the axis will pass through the focal point.

• A ray that initially has a direction thatpasses through the focal point will emerge parallel to the central axis.

• A ray going through the center of thelens will be undeflected.

• The image of a point appears where all rays emanating from a point intersect.

Page 9: Lecture 25 - phys.lsu.eduphys.lsu.edu/~jdowling/PHYS21024SP07/lectures/lecture25.pdf · Lecture 25 Physics 2102 Jonathan Dowling Optics: Images. Thin Lenses pif 111 += For small angles

Images due to lenses:

• An object placed beyond a convergent lenses’ focal point, will producea real, inverted image on the other side of the lens. This is the principleused in slide projectors.

• An object placed between a convergent lens and its focal point willproduce a virtual image on the same side as the object.

•Divergent lenses always produce a virtual image on the same side asthe object.

• Real images have i positive in formulas, virtual images have i negative.

Page 10: Lecture 25 - phys.lsu.eduphys.lsu.edu/~jdowling/PHYS21024SP07/lectures/lecture25.pdf · Lecture 25 Physics 2102 Jonathan Dowling Optics: Images. Thin Lenses pif 111 += For small angles

ExampleExample• An object 2cm high is placed 4cm from a bi-convex lens withr1=10cm and r2=15cm, and index of refraction n=1.5. Find theposition and size of the image.

• A second lens of focal length +6cm is placed 12cm to the right ofthe first lens. Find the position and size of the new image.

Page 11: Lecture 25 - phys.lsu.eduphys.lsu.edu/~jdowling/PHYS21024SP07/lectures/lecture25.pdf · Lecture 25 Physics 2102 Jonathan Dowling Optics: Images. Thin Lenses pif 111 += For small angles

The human eyeThe human eye consists of avariable-geometry lens (crystalline)which produces a real image on a“screen” (retina) which is transmittedto the brain via the optical nerve.

The cristalline automatically adjusts itself so we see well any objectplaced between infinity and a distance called “near point” (about 25cmfor a typical 20 year old). The “image distance” is the eye diameter~2cm.

Optical Instruments: the human eyeOptical Instruments: the human eye

Page 12: Lecture 25 - phys.lsu.eduphys.lsu.edu/~jdowling/PHYS21024SP07/lectures/lecture25.pdf · Lecture 25 Physics 2102 Jonathan Dowling Optics: Images. Thin Lenses pif 111 += For small angles

Optical instruments: combinationOptical instruments: combinationof several (thin) lensesof several (thin) lenses

F1 F1

F2 F2

If lenses are very close, the compound lens has 1/f~1/f1+1/f2

Page 13: Lecture 25 - phys.lsu.eduphys.lsu.edu/~jdowling/PHYS21024SP07/lectures/lecture25.pdf · Lecture 25 Physics 2102 Jonathan Dowling Optics: Images. Thin Lenses pif 111 += For small angles

Corrective GlassesCorrective Glasses

A farsighted person needs a convergent lens.

A nearsighted person needs a divergent lens.

The “power” of a lens is measured in dioptres: P=1/f with f is in m.Glasses with -6D are divergent glasses with f=−1/6D =−0.17m=−17cmThe dioptres add! Two lenses have 1/f=1/f1+1/f2 → D=D1+D2

Page 14: Lecture 25 - phys.lsu.eduphys.lsu.edu/~jdowling/PHYS21024SP07/lectures/lecture25.pdf · Lecture 25 Physics 2102 Jonathan Dowling Optics: Images. Thin Lenses pif 111 += For small angles

The magnification of an object is m=i/p~iθ/h,but i=eye diameter.Maximum magnification: m~2cm/25cm (!?)

Angular magnification (different from lateral): mθ=θ’/θ.

f

cm

f

h

cm

h 25m '

25=!= """

Magnifying lensMagnifying lens

We’d like to make p smaller (move the object closer). We use amagnifying lens to produce a (larger) image than our eye can see:

Very near the focus!

Page 15: Lecture 25 - phys.lsu.eduphys.lsu.edu/~jdowling/PHYS21024SP07/lectures/lecture25.pdf · Lecture 25 Physics 2102 Jonathan Dowling Optics: Images. Thin Lenses pif 111 += For small angles

Microscope:

To increase the magnification of a lens, one wants to have a shortfocal length. That means small radii of curvature (very curved lens).This, in turn implies a lot of aberration (one is immediately out ofthe thin lens approximation). A solution to this is obtained bycombining two lenses. The resulting device is called microscope.

p

im !=

Object O is magnifiedby the objective:

And its image is magnifiedby the eyepiece:

f

cmm

25=!

Total magnification:

eyob f

cm

f

smmM

25!== "

Page 16: Lecture 25 - phys.lsu.eduphys.lsu.edu/~jdowling/PHYS21024SP07/lectures/lecture25.pdf · Lecture 25 Physics 2102 Jonathan Dowling Optics: Images. Thin Lenses pif 111 += For small angles

Telescope:

Telescopes are arrangement of lenses that improve vision of objectsvery far away. They are configured like a microscope. However, theobjective forms an image essentially at its focus, and therefore theeyepiece’s focus has to be placed at that same point.

The magnification is given bythe ratio θey/θob, and since

obob fh /'=! eyey fh /'=!

ey

ob

f

fm !=

Refracting telescopes are of limiteduse (chromatic aberration). Reflectingtelescopes built with mirrors are preferred in astronomy.

Page 17: Lecture 25 - phys.lsu.eduphys.lsu.edu/~jdowling/PHYS21024SP07/lectures/lecture25.pdf · Lecture 25 Physics 2102 Jonathan Dowling Optics: Images. Thin Lenses pif 111 += For small angles

ExampleExampleThe world’s largest refracting telescope is at the YerkesObservatory of the University of Chicago at Williams Bay,Wisconsin. The objective has a diameter of 102cm and a focallength of 19.5m. The focal length of the eyepiece is 10cm. What isits magnifying power?

1951.0

5.19!=!=!=

m

m

f

fm

ey

ob

Why so large (102cm)? Because thelarger the objective, the more light itgathers.

Page 18: Lecture 25 - phys.lsu.eduphys.lsu.edu/~jdowling/PHYS21024SP07/lectures/lecture25.pdf · Lecture 25 Physics 2102 Jonathan Dowling Optics: Images. Thin Lenses pif 111 += For small angles

Reflective telescopesReflective telescopes

Keck observatory (MaunaKea, Hawaii) and theHale-Bopp comet.

Largest optical telescope,composed of 36 (!)hexagonal mirrorsegments performing as asingle mirror 10m wide.