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電磁波基本性質實驗

電磁波基本性質實驗. Bragg Diffraction ( 布拉格繞射 ) Fiber Optics ( 光纖光學 ). Bragg Diffraction ( 布拉格繞射 ). 由相鄰 兩晶面 所反射出來的電磁波之 波程差 若為 2dsin  , 其中 d 為 晶面距離 ,  為入射波與 晶面 之間夾角 , 則 建設性干涉 的條件為 波程差 恰好為 波長 λ 的整數倍 : 2dsin  = n λ  n = 1, 2, 3 … 布拉格定律 ( Bragg’s Law). Diffraction of X-Rays by Crystals.

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電磁波基本性質實驗

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  1. 電磁波基本性質實驗 • Bragg Diffraction (布拉格繞射) • Fiber Optics(光纖光學)

  2. Bragg Diffraction (布拉格繞射) • 由相鄰兩晶面所反射出來的電磁波之波程差若為 2dsin,其中d 為晶面距離,為入射波與晶面之間夾角,則建設性干涉的條件為波程差恰好為波長λ的整數倍 : 2dsin = nλn = 1, 2, 3 … 布拉格定律(Bragg’s Law)

  3. Diffraction of X-Rays by Crystals Laue pattern

  4. Laue Pattern for Beryl(Beryllium aluminum silicate)

  5. Laue Pattern for enzyme Rubisco

  6. z y x Crystalline structure of Nacl Na+ Cl- Fig. 27-27, p. 920

  7. 晶面之指數(Miller indics) • 晶面上的三點決定晶面之指數(Miller indics) • 三個晶軸與晶面交接點(截距) • 取截距倒數 • 化成最小整數比

  8. ( 1 0 0 )平面 z y ( 2 0 0 ) 平面 ( 1 0 0 ) 平面 x

  9. ( 1 1 0 )平面 z y x

  10. ( 1 1 1 )平面

  11. Bragg Diffraction (布拉格繞射)  2  2dsin = nλn = 1, 2, 3 … Fig. 27-28, p. 920

  12.   2 發射器 2dsin = nλn = 1, 2, 3 … Grazing angle d 接收器 接收器

  13. (210)面 1 2

  14. Fiber Optics(光纖光學) • 利用細長柔軟纖維(由玻璃、塑膠或其他透明材料製成)傳送光信號的技術 • 光波由纖維絲的一端進入後,由於全反射作用,將纖維絲方向傳輸而不從周壁逸出

  15. Snell’s Law of Refraction • Snell’s Law • n1 sin θ1 = n2 sin θ2 • θ1 is the angle of incidence • θ2 is the angle of refraction n1 n2

  16. Total Internal Reflection • A phenomenon called total internal reflection can occur when light is directed from a medium having a given index of refraction toward one having alower index of refraction

  17. Critical Angle • There is a particular angle of incidence that will result in an angle of refraction of 90° • This angle of incidence is called the critical angle, θC

  18. Optical Fibers • An application of internal reflection • Plastic or glass rods are used to “pipe” light from one place to another • Applications include • medical use of fiber optic cables for diagnosis and correction of medical problems • Telecommunications

  19. Optical Fibers, cont • A flexible light pipe is called an optical fiber • A bundle of parallel fibers (shown) can be used to construct an optical transmission line

  20.  接收器 R-d 發射器

  21. End of the Lecture

  22. Optical Fibers, cont • A flexible light pipe is called an optical fiber • A bundle of parallel fibers (shown) can be used to construct an optical transmission line

  23. Construction of an Optical Fiber • The transparent core is surrounded by cladding • The cladding has a lower n than the core • This allows the light in the core to experience total internal reflection • The combination is surrounded by the jacket

  24. Multimode, Stepped Index Fiber • Stepped index comes from the discontinuity in n between the core and the cladding • Multimode means that light entering the fiber at many angles is transmitted

  25. Multimode, Graded Index Fiber • This fiber has a core whose index of refraction is smaller at larger radii from the center • The resultant curving reduces transit time and reduces spreading out of the pulse

  26. Optical Fibers, final • Optical fibers can transmit about 95% of the input energy over one kilometer • Minimization of problems includes using as long a wavelength as possible • Much optical fiber communication uses wavelengths of about 1300 nm.

  27. Total Internal Reflection (Critical Angle) • There is a particular angle of incidence that will result in an angle of refraction of 90° • This angle of incidence is called the critical angle, θC

  28.  R-d 產生Total Internal Reflection

  29. Fig. 25-28, p. 856

  30. Fig. 25-29, p. 857

  31. Fig. 25-30, p. 857

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