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Pertemuan 4-5 Fisika Modern Basic Atomic Physics Hadi Nasbey, M.Si ,[object Object],[object Object],07/03/11 ©  2010 Universitas Negeri Jakarta  |  www.unj.ac.id  |
Outline ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],07/03/11 ©  2010 Universitas Negeri Jakarta  |  www.unj.ac.id  |
K α 07/03/11 ©  2010 Universitas Negeri Jakarta  |  www.unj.ac.id  | n=4 n=3 n=2 n=1 K γ K β L β L α L γ N=5
[object Object],07/03/11 ©  2010 Universitas Negeri Jakarta  |  www.unj.ac.id  |
[object Object],[object Object],[object Object],07/03/11 ©  2010 Universitas Negeri Jakarta  |  www.unj.ac.id  |
-ve electrode +ve electrode 07/03/11 ©  2010 Universitas Negeri Jakarta  |  www.unj.ac.id  |
E=eV X-Ray Ejected electron 07/03/11 ©  2010 Universitas Negeri Jakarta  |  www.unj.ac.id  |
07/03/11 For K transitions For any transitions Continuous spectrum Line spectrum ©  2010 Universitas Negeri Jakarta  |  www.unj.ac.id  |
07/03/11 ©  2010 Universitas Negeri Jakarta  |  www.unj.ac.id  |
[object Object],,   =   K , L, M If, however, the electron loses a certain amount of energy by collision in the target before producing X-radiation, its energy when it radiates is less than the maximum possible energy,   ›  0   07/03/11 ©  2010 Universitas Negeri Jakarta  |  www.unj.ac.id  |
[object Object],[object Object],[object Object],[object Object],07/03/11 ©  2010 Universitas Negeri Jakarta  |  www.unj.ac.id  |
Becquerel   discovered while working with uranium salts that they emitted particles or radiation which could affect photographic plates. Rutherford  and others began an extensive investigation of the phenomenon, the main lines of research being into (a) what sort of particles were being emitted,  (b)what sort of laws the emission mechanism obeyed . 07/03/11 ©  2010 Universitas Negeri Jakarta  |  www.unj.ac.id  |
[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],07/03/11 ©  2010 Universitas Negeri Jakarta  |  www.unj.ac.id  |
07/03/11 ©  2010 Universitas Negeri Jakarta  |  www.unj.ac.id  |
[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],07/03/11 ©  2010 Universitas Negeri Jakarta  |  www.unj.ac.id  |
07/03/11 Here T 1/2  is the half-life, the time it takes for half the nuclei to decay - i.e. for A to decrease to A/2.  Here    is called the average lifetime. A=Activity=  N A (t) =½ A o ,  at t=T 1/2      - Units  time -1  (s -1,  d -1 , m -1 , y -1 ) ©  2010 Universitas Negeri Jakarta  |  www.unj.ac.id  |
N o -N(t)= N o ( 1- e -  t  )  07/03/11 ©  2010 Universitas Negeri Jakarta  |  www.unj.ac.id  | 14 C  14 N
Ln N(t)= Ln N o  -  t Ln x = 2.3 Log x 07/03/11 ©  2010 Universitas Negeri Jakarta  |  www.unj.ac.id  | Ln N(t)  Ln N o   Time, t
[object Object],The main processes by which X- and  γ -rays are absorbed are  photo­electric effect   Pair production Lead Shield Lead Shield Compton Effect Ln I= Ln I o - µx Detector 07/03/11 ©  2010 Universitas Negeri Jakarta  |  www.unj.ac.id  | I 0 I (x ) x
+ - Pair production 07/03/11 ©  2010 Universitas Negeri Jakarta  |  www.unj.ac.id  | E=hƒ E”=hƒ” Compton Photoelectric
I (x)  = I 0  e -µx   07/03/11 ©  2010 Universitas Negeri Jakarta  |  www.unj.ac.id  |
Ln I= Ln I o - µx 07/03/11 ©  2010 Universitas Negeri Jakarta  |  www.unj.ac.id  |
[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],07/03/11 ©  2010 Universitas Negeri Jakarta  |  www.unj.ac.id  |
5-3 Radiation Units roentgen  (R) •  measures exposure (ionization) of air by X-rays & gamma-rays Quantity of x-rays which loses 8.34x10 -7 j/g of air rad   (radiation absorbed dose) •  measures energy deposited in any material by any type of ionizing radiation 1   rad  = 0.01 J/kg   07/03/11 ©  2010 Universitas Negeri Jakarta  |  www.unj.ac.id  |
[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],07/03/11 ©  2010 Universitas Negeri Jakarta  |  www.unj.ac.id  |
[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],07/03/11 ©  2010 Universitas Negeri Jakarta  |  www.unj.ac.id  |
[object Object],[object Object],07/03/11 ©  2010 Universitas Negeri Jakarta  |  www.unj.ac.id  |
Terrestrial Sources 5-4 Radiation hazards The average annual dose to the general  population from natural background  and man-made sources is 360 mrem. Cosmic Radiation Internal Sources Other Radon Radon 07/03/11 ©  2010 Universitas Negeri Jakarta  |  www.unj.ac.id  |
[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],07/03/11 ©  2010 Universitas Negeri Jakarta  |  www.unj.ac.id  |
Time 5-5 Radiation Protection Distance Shielding All workers are required to wear film badges or pocket ionization chambers which, are checked regularly to calculate dosages received 07/03/11 ©  2010 Universitas Negeri Jakarta  |  www.unj.ac.id  |
TERIMA KASIH 07/03/11 ©  2010 Universitas Negeri Jakarta  |  www.unj.ac.id  |

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Fisika Modern 04 basic atomicphysics

  • 1.
  • 2.
  • 3. K α 07/03/11 © 2010 Universitas Negeri Jakarta | www.unj.ac.id | n=4 n=3 n=2 n=1 K γ K β L β L α L γ N=5
  • 4.
  • 5.
  • 6. -ve electrode +ve electrode 07/03/11 © 2010 Universitas Negeri Jakarta | www.unj.ac.id |
  • 7. E=eV X-Ray Ejected electron 07/03/11 © 2010 Universitas Negeri Jakarta | www.unj.ac.id |
  • 8. 07/03/11 For K transitions For any transitions Continuous spectrum Line spectrum © 2010 Universitas Negeri Jakarta | www.unj.ac.id |
  • 9. 07/03/11 © 2010 Universitas Negeri Jakarta | www.unj.ac.id |
  • 10.
  • 11.
  • 12. Becquerel discovered while working with uranium salts that they emitted particles or radiation which could affect photographic plates. Rutherford and others began an extensive investigation of the phenomenon, the main lines of research being into (a) what sort of particles were being emitted, (b)what sort of laws the emission mechanism obeyed . 07/03/11 © 2010 Universitas Negeri Jakarta | www.unj.ac.id |
  • 13.
  • 14. 07/03/11 © 2010 Universitas Negeri Jakarta | www.unj.ac.id |
  • 15.
  • 16. 07/03/11 Here T 1/2 is the half-life, the time it takes for half the nuclei to decay - i.e. for A to decrease to A/2. Here  is called the average lifetime. A=Activity=  N A (t) =½ A o , at t=T 1/2  - Units time -1 (s -1, d -1 , m -1 , y -1 ) © 2010 Universitas Negeri Jakarta | www.unj.ac.id |
  • 17. N o -N(t)= N o ( 1- e -  t ) 07/03/11 © 2010 Universitas Negeri Jakarta | www.unj.ac.id | 14 C 14 N
  • 18. Ln N(t)= Ln N o -  t Ln x = 2.3 Log x 07/03/11 © 2010 Universitas Negeri Jakarta | www.unj.ac.id | Ln N(t) Ln N o Time, t
  • 19.
  • 20. + - Pair production 07/03/11 © 2010 Universitas Negeri Jakarta | www.unj.ac.id | E=hƒ E”=hƒ” Compton Photoelectric
  • 21. I (x) = I 0 e -µx 07/03/11 © 2010 Universitas Negeri Jakarta | www.unj.ac.id |
  • 22. Ln I= Ln I o - µx 07/03/11 © 2010 Universitas Negeri Jakarta | www.unj.ac.id |
  • 23.
  • 24. 5-3 Radiation Units roentgen (R) • measures exposure (ionization) of air by X-rays & gamma-rays Quantity of x-rays which loses 8.34x10 -7 j/g of air rad (radiation absorbed dose) • measures energy deposited in any material by any type of ionizing radiation 1 rad = 0.01 J/kg 07/03/11 © 2010 Universitas Negeri Jakarta | www.unj.ac.id |
  • 25.
  • 26.
  • 27.
  • 28. Terrestrial Sources 5-4 Radiation hazards The average annual dose to the general population from natural background and man-made sources is 360 mrem. Cosmic Radiation Internal Sources Other Radon Radon 07/03/11 © 2010 Universitas Negeri Jakarta | www.unj.ac.id |
  • 29.
  • 30. Time 5-5 Radiation Protection Distance Shielding All workers are required to wear film badges or pocket ionization chambers which, are checked regularly to calculate dosages received 07/03/11 © 2010 Universitas Negeri Jakarta | www.unj.ac.id |
  • 31. TERIMA KASIH 07/03/11 © 2010 Universitas Negeri Jakarta | www.unj.ac.id |