第10章-几何光学课件.ppt
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1、 几何光学是以光的直线传播性质为基础,几何光学是以光的直线传播性质为基础,研究光在透明介质中传播规律的学科。研究光在透明介质中传播规律的学科。光光 的的 直直 线线 传传 播播 定定 律律光光 的的 独独 立立 传传 播播 定定 律律反射和折射定律反射和折射定律几几何何光光学学的的理理论论基基础础1Section 1.Refraction at a Spherical Surface Section 1.Refraction at a Spherical Surface Section 2.The lensSection 2.The lensSection 3.The eye Section
2、3.The eye Section 4.The Magnifier and MicroscopeSection 4.The Magnifier and MicroscopeSection 5.The Special Microscope and FiberscopesSection 5.The Special Microscope and Fiberscopes21.Refraction at a Spherical Surface2.Coaxial SystemSection 1.Refraction at a Spherical Surface Section 1.Refraction a
3、t a Spherical Surface 3n1n2uvobjectimagerCrn1i1i2APParaxial condition,i1 i2 analyze球面折射系统球面折射系统1.Refraction at a Spherical Surface 1.Refraction at a Spherical Surface 5 discussCondition:Paraxial beamWe adopt the following rules:1、When the object is on the same side of the refracting surface as the i
4、ncoming light,the object distance u is positive;otherwise it is negative.球面折射系统球面折射系统1.Refraction at a Spherical Surface 1.Refraction at a Spherical Surface 2、When the image is on the same side of the refracting surface as the outgoing light,the image distance v is positive;otherwise it is negative.
5、61.Refraction at a spherical surface1.Refraction at a spherical surface 3、When the center of curvature C is on the same side as the outgoing light,the radius of curvature is positive;otherwise it is negative.Dioptric power(D)R:metersA quantity of describing the ability of refraction For the refracti
6、ve system :(diopter)7n1n2CrPrimary focal pointF1f1Primary focal length1.Refraction at a Spherical Surface1.Refraction at a Spherical Surface 8focusPrimary focal pointPrimary focal length Secondary focal pointSecondary focal lengthImage is at the infinityObject is at the infinityFocal degree 球面折射系统球面
7、折射系统(diopter-D)102.Coaxial systemApplying the methods of single spherical refraction in turn,the object for the second surface being the image formed by the first.12Example A glass ball(n=1.5)which diameters is 20cm.A object is put at the place of 40cm before the sphere.Where is the image?To the fir
8、st refractive surface n11.0,n21.5,u140cm,r10cm,60cm 14To the second refractive surface u2(60-20)40cm,n11.5,n21.0,r10cm,11.4cm151.The Thin-lens Equation2.The Combination of the thin lens3.The Thick lens4.The cylindrical lens5.Lens AberrationsSection 2 The lens Section 2 The lens 16LensBe made up of t
9、wo coaxial refractive surfaceIncluding(converging lens and diverging lens)Two refractive surface are all spherical surfaces,or one is spherical surface,another one is plane。The distance on the optic axis between the two refractive surface is lens thicknessThin lens The lens thickness is negligible i
10、n comparison with the object distance and the image distance Thick lens薄透镜薄透镜1.The thin-lens Equation171).The lines through the center of the lens dont change direction.2).The parallel light lays with the axis pass through the focal point after refraction;3).The light rays through focal point is par
11、allel with the Axis after refraction。FOF薄透镜薄透镜Basic imaging law about thin lens18To the first refractive surface To the second refractive surface u=u1 n1 v=v2 v1=u2+薄透镜薄透镜20 u=u1 v=v2 n1 v1=u2+n1n2薄透镜薄透镜 Gauss Equation about thin-lens 21Converging lensDiverging lens r1 0 r2 0 r1 0 f 0薄透镜薄透镜23Dioptri
12、c power 表示透镜的折光本领表示透镜的折光本领unit:diopter (屈光度)屈光度)通常所说的眼镜的度数等于屈光度的通常所说的眼镜的度数等于屈光度的1/100倍倍1屈光度屈光度=100度度D越大,系统的折光能力越强越大,系统的折光能力越强薄透镜薄透镜24Example 10-3p191(板书讲板书讲)26 The coaxial system is made up of two or more thin lens。DefinitionsConstructImaging in turn Equation薄透镜薄透镜2.The combination of thin lens 27To
13、 the first lensTo the second lens u=u1 v=v2 v1=-u2+薄透镜薄透镜283 3、Thick Lens Thick Lens1).Concept of thick lens2).Imaging law30The term thick lens means either a single lens whose thickness is not negligible in comparison with the object distance and the image distance,or any combination of lens such a
14、s a corrected camera lens.Thick lens1).ConceptThin lens31 对每一个单球面,依次应用单球面系统的成像对每一个单球面,依次应用单球面系统的成像规律;规律;利用共轴系统的基点概念利用共轴系统的基点概念把透镜看做是一把透镜看做是一个体系,定义这个系统的三对基点,只要知道这三个体系,定义这个系统的三对基点,只要知道这三对基点的位置,就可以用作图法解决成像问题对基点的位置,就可以用作图法解决成像问题;Thick lens方法一方法一方法二方法二*计算法解决一些成像问题。计算法解决一些成像问题。-Imaging equation方法三方法三2).Im
15、aging law32a).Two focal point 调整光源在主光轴上的位置,使其光束通过厚透调整光源在主光轴上的位置,使其光束通过厚透镜后变为平行光,这时点光源所在的位置就称为共轴镜后变为平行光,这时点光源所在的位置就称为共轴系统的第一主焦点系统的第一主焦点F1。平行于主光轴的光束,通过系统折射后与主光轴平行于主光轴的光束,通过系统折射后与主光轴相交于一点,称为共轴系统的第二主焦点相交于一点,称为共轴系统的第二主焦点F2。The primary principal focal pointF1The secondary principal focal pointF2Thick lens
16、33b).Two principal points 通过通过F1的入射光线的延长线与出射光线的反的入射光线的延长线与出射光线的反向延长线交于向延长线交于A1点,过点,过A1点所做的垂直于主光轴点所做的垂直于主光轴的平面称为共轴系统的第一主平面,第一主平面的平面称为共轴系统的第一主平面,第一主平面与光轴的交点与光轴的交点H1就称为共轴系统的第一主点。就称为共轴系统的第一主点。平行于主光轴的入射光线与其射出线的平行于主光轴的入射光线与其射出线的反向延长线的交点,决定了系统的第二主平反向延长线的交点,决定了系统的第二主平面,第二主点。面,第二主点。F1F2H1A1H2Thick lens34 不管光
17、线在厚透镜中经过怎样曲析的路径,不管光线在厚透镜中经过怎样曲析的路径,在效果上可以看作只在主平面上发生折射。在效果上可以看作只在主平面上发生折射。F1F2H1H2 通过一个主平面上任一点的光线,一定通通过一个主平面上任一点的光线,一定通过另一主平面上的对应点。过另一主平面上的对应点。Thick lens Two principal points 35c).Two nodal points There are another two points N1 and N2,called nodal points which are similar as the optical center of th
18、in lens that rays pass through them without deviated as in next fig.Here QN1 is parallel to QN2.Thick lensN1N2F1F2H1H2QQ 36方法二方法二 厚透镜的基点作图法厚透镜的基点作图法 N1N2F1F2H1H2 通过第一主焦点的光线在第一主平面上折射通过第一主焦点的光线在第一主平面上折射后平行主光轴射出;后平行主光轴射出;平行于主光轴的光线在第二主平面折射后,平行于主光轴的光线在第二主平面折射后,通过第二主焦点;通过第二主焦点;通过第一节点的光线从第二节点平行于入射通过第一节点的光线
19、从第二节点平行于入射方向射出。方向射出。Thick lens371.A ray parallel to the axis is refracted by the second principal plane and passes through the second focal point of a thick lens.2.A ray through the first focal point is refracted by the first principalplane and emerges parallel to the axis.3.A ray through the first
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