• Tidak ada hasil yang ditemukan

PDF Light: Basic principles - Seoul National University

N/A
N/A
Protected

Academic year: 2024

Membagikan "PDF Light: Basic principles - Seoul National University"

Copied!
16
0
0

Teks penuh

(1)(2) (3) (4) (5)  Frequency (Hz).  Wavelength (m). 10 22. 10. h Photon energy (eV). h Photon energy (J) -RAYS. 13. 1MeV. 10. 6. 10 14. 1Å 1nm 1015 1014. 1THz. 1mm. 1MHz. 1kHz. 10 10 10 9. 10 6. 1keV. 10. X-RAYS. 3. ULTRAVIOLET 1eV. 10 100 101. 10 18 LIGHT 10 19 10 20 INFRARED. 1012. 1cm 1GHz. MICROSCOPIC SOURCE. 10. 9. 106. 103. 1m 1km. 10. MICROWAVES. 2. 21cm H line. 100. 106. 10. 10 2 103 105. UHF VHF TV. 1011. 27. Radar FM Radio Broadcast. RADIOFREQUENCY Power Lines. ARTTIFICIAL DETECTION GENERATION. Atomic nuclei. Geiger and scintillation. Accelerators. Inner electrons. Ionization chamber. X-ray tubes. Inner and Outer electrons Outer electrons Molecular vibrations and rotations Electron spin Nuclear spin. Photoelectric Photomultiplie r Eye Bolometer. Synchrotrons Lasers Arcs Sparks Lamps. Thermopile. Hot bodies. Crystal. Magnetron Klystron Travelling-wave tube. Electronic circuits. Electronic circuits. AC generators. (6) B 0 t D H  J t D   E . . B  0. D  E   o E  P H. B. m. . B. mo. M. . (7)  2E  2H 2  E  m 2  0,  H  m 2  0 t t 2. e.g. f ( x, t )  f ( x   x, t   t ).   ei (t kr ) , k   m. t  k  r  constant, v p  c. 1. m o o.  k. .  2.997930 108 m / s. 1. m. ,. (8) B E   0  n  (E 2  E1 )  0  t D H   J  n  ( H 2  H1 )  K  t  n  (D 2  D1 )    D   B  0. . n  (B 2  B1 )  0. . (9) q q. q q. q. q. ni sin q i  nt sin q t. . (10) 1.0. 1.0. 0.8 ni < nt ni = 1, nt = 1.5. 0.6. Reflectivity. Reflectivity. 0.8. P-Polarization S-Polarization. 0.4. ni > n t ni = 1.5, nt = 1. 0.6. P-Polarization S-Polarization. 0.4 0.2. 0.2. 0.0. 0.0 0. 10 20 30 40 50 60 70 80 90. 0. 10 20 30 40 50 60 70 80 90 Incident Angle qi [deg]. Incident Angle qi [deg]. nt q B  tan ( ) ni 1.  qi  qt  .  2. n ni. q c  sin 1 ( t )  ni  nt , q t  .  2. (11) D  E   o E  P.  nx2     o 0 0 . 0 n y2 0. 0  0 nz2 .  nx  n y  nz  Isotropic   nx  n y  nz  Uniaxial  n  n  n  Biaxial y z  x. (12) ni sin q i  nt sin q t. (13) . . ~. 1. 4. (14) (15) . (16)  2nd cos q  m. (17)

Referensi

Dokumen terkait

Therefore, the objectives of the present study were to 1 examine the changes in the trajectories of cognitive function and identify the risk factors that influence these changes, 2 to

2.5.2 Change in s-s The change of strain due to creep and shrinkage of concrete and relaxation of prestressed steel is first artificially restrained by application of axial force and

The purpose of this paper is to show that even in the cases of Ross' Relative Clause Formation and Lakoff's It-Replacement, the arguments for the necessity of Chomsky- adjunction are

Nucleation and Growth Rates – Good Glass Formers  No overlap of growth and nucleation rates  Nucleation rate is small  Growth rate is small  At any one temperature one of the

Ch 1,2 Sl 16 Molar mass [ 分子量 ]  polymer is ‘molecule with high molar mass’  molar mass vs molecular weight  [g/mol] vs dimensionless or [g/molecule]  MM preferred over MW 

“Bending stress” or “flexural stress” is proportional to the bending moment 𝑀𝑀 and inversely proportional to the moment of inertia 𝐸𝐸; The stress varies linearly with the distance 𝑦𝑦

1 Fundamental Principles of Mechanics 3 / 14 1.3 Fundamental Principles of Mechanics u Two different types of movement which are important in the mechanics of solids i Gross

In the overhead output stream, the benzene flow rate is 36kg/hr, and in the bottoms output stream, the tolune flow rate is 54kg/hr.. What are the toluene flow rate in the overhead