Kuliah Elektronika Dasar Minggu ke 4 DIODA

Presentasi berjudul: "Kuliah Elektronika Dasar Minggu ke 4 DIODA"— Transcript presentasi:

1 Kuliah Elektronika Dasar Minggu ke 4 DIODA
Jurusan Teknik Elektro Fakultas Teknik UGM 2007

2 FUNCTION + - - + Electrical ‘gate’ Forward biased Reverse biased
Current only flows one way Forward biased Current flows Reverse biased Blocks current + - - +

3 I-V characteristic Forward Bias Breakdown Voltage
Reverse saturation current 0.7V Switch-on Reverse Bias

4 PN CONSTRUCTION Semiconductor material n-type p-type ‘Join’ together
Excess electrons p-type Excess holes ‘Join’ together Depletion region Redistribution of charge carriers Contact potential 0.7V

5 SAMBUNGAN PN p-type material n-type material
Holes diffuse into the n-type and ‘swallow’ electrons Electrons diffuse into the p-type and ‘fill holes’ Depletion region formed No free charge carriers 0.7V contact potential

6 FORWARD BIAS + P N Applied voltage above 0.7V
depletion region is removed charge carriers can flow Depletion region narrows as applied voltage approaches 0.7V Depletion Region V< 0.7V V> 0.7V P N + DAERAH DEPLESI MENYEMPIT  MENGHILANG

7 REVERSE BIAS Depletion region extends Higher voltage + + V<< 0V
Breakdown Current flow V< 0V V<< 0V + + DAERAH DEPLESI MELEBAR  MAKIN LEBAR

8 Bohr model (I hope it’s not bohring)
The Bohr model is a planetary model, where the electron orbits the nucleus like a planet orbits the Sun. An electron is only allowed in DISCRETE orbits (n=1, n=2, n=3, etc.) The higher the orbit, the higher the energy of the electron.

9 PITA ENERGI SEBUAH ATOM
PITA HANTARAN CELAH ENERGI PITA VALENSI INTI

10 PITA ENERGI PITA HANTARAN PITA HANTARAN PITA HANTARAN PITA VALENSI
No Gap PITA HANTARAN Large Gap PITA HANTARAN Small Gap PITA VALENSI PITA VALENSI PITA VALENSI Insulators Metals Semiconductors

11 Elektron di orbit terluar
Silicon Tetravalent Boron Trivalent “Acceptor” Phosphorus Pentavalent “Donor”

12 PITA ENERGI PITA HANTARAN celah energi PITA VALENSI elektron

13 Jumlah Elektron Bebas = Jumlah Hole
TERBENTUKNYA HOLE PITA HANTARAN ELEKTRON BEBAS ENERGI TAMBAHAN elektron PITA VALENSI HOLE Jumlah Elektron Bebas = Jumlah Hole

14 P-N JUNCTION FORMATION
p-type material Semiconductor material doped with acceptors. Material has high hole concentration Concentration of free electrons in p-type material is very low. n-type material Semiconductor material doped with donors. Material has high concentration of free electrons. Concentration of holes in n-type material is very low.

15 P-N JUNCTION FORMATION
p-type material Contains NEGATIVELY charged acceptors (immovable) and POSITIVELY charged holes (free). Total charge = 0 n-type material Contains POSITIVELY charged donors (immovable) and NEGATIVELY charged free electrons. Total charge = 0

16 P-N JUNCTION FORMATION
What happens if n- and p-type materials are in close contact? p-type material Contains NEGATIVELY charged acceptors (immovable) and POSITIVELY charged holes (free). Total charge = 0 n-type material Contains POSITIVELY charged donors (immovable) and NEGATIVELY charged free electrons. Total charge = 0

17 p- n junction formation
What happens if n- and p-type materials are in close contact? Being free particles, electrons start diffusing from n-type material into p-material Being free particles, holes, too, start diffusing from p-type material into n-material Have they been NEUTRAL particles, eventually all the free electrons and holes had uniformly distributed over the entire compound crystal. However, every electrons transfers a negative charge (-q) onto the p-side and also leaves an uncompensated (+q) charge of the donor on the n-side. Every hole creates one positive charge (q) on the n-side and (-q) on the p-side

18 p- n junction formation
What happens if n- and p-type materials are in close contact? p-type n-type Electrons and holes remain staying close to the p-n junction because negative and positive charges attract each other. Negative charge stops electrons from further diffusion Positive charge stops holes from further diffusion The diffusion forms a dipole charge layer at the p-n junction interface. There is a “built-in” VOLTAGE at the p-n junction interface that prevents penetration of electrons into the p-side and holes into the n-side.

19 p- n junction current – voltage characteristics
What happens when the voltage is applied to a p-n junction? p-type n-type The polarity shown, attracts holes to the left and electrons to the right. According to the current continuity law, the current can only flow if all the charged particles move forming a closed loop However, there are very few holes in n-type material and there are very few electrons in the p-type material. There are very few carriers available to support the current through the junction plane For the voltage polarity shown, the current is nearly zero

20 p- n junction current – voltage characteristics
What happens if voltage of opposite polarity is applied to a p-n junction? p-type n-type The polarity shown, attracts electrons to the left and holes to the right. There are plenty of electrons in the n-type material and plenty of holes in the p-type material. There are a lot of carriers available to cross the junction. When the voltage applied is lower than the built-in voltage, the current is still nearly zero When the voltage exceeds the built-in voltage, the current can flow through the p-n junction

21 Diode current – voltage (I-V) characteristics
Semiconductor diode consists of a p-n junction with two contacts attached to the p- and n- sides p n V IS is usually a very small current, IS ≈ …10-13 A When the voltage V is negative (“reverse” polarity) the exponential term ≈ -1; The diode current is ≈ IS ( very small). When the voltage V is positive (“forward” polarity) the exponential term increases rapidly with V and the current is high.

22 Δίοδος

23 p-n junction formation
p-type material Semiconductor material doped with acceptors. Material has high hole concentration Concentration of free electrons in p-type material is very low. n-type material Semiconductor material doped with donors. Material has high concentration of free electrons. Concentration of holes in n-type material is very low.

24 IKATAN KOVALENT

25 SILIKON DIPANASI

26 DI DOPING ATOM BERVALENSI 5
BAHAN N ION POS

27 DI DOPING ATOM BERVALENSI 3
BAHAN P ION NEG

28 DI DOPING ATOM BERVALENSI 5
BAHAN N ION POS

29 DI DOPING ATOM BERVALENSI 3
BAHAN P ION NEG

30 BAGAIMANA MEMBUAT BAHAN N ?
Bahan silikon diberi doping atom bervalensi 5 (misal : pospor) Atom pospor disebut DONOR Uap pospor N Si RUANG HAMPA

31 Bahan semikonduktor jenis P
Bahan silikon diberi doping atom bervalensi 3 (misal : boron) Atom boron disebut ASEPTOR Uap boron P Si RUANG HAMPA

32 DISTRIBUSI HOLE

33 TEGANGAN KONTAK

34 Simbul dioda dan arah arus
Karakteristik ideal Rangkaian ekivalen saat forward bias Rangkaian ekivalen saat reverse bias

35 PENDEKATAN IDEAL

36 p- n diode applications:
current rectifiers - + + - Voltage Current Time Time

37 PENYEARAH setengah gelombang
Tegangan input Saat forward π 2π Tegangan output Saat reverse

38 TEGANGAN DC RATA-RATA Mengintegralkan satu periode VDC 2π

39 Bila ada tegangan lawan

40 Contoh rangkaian dioda

41 MELIHAT DETIL

42 PENGARUH PANAS

43 GARIS KERJA (load line)

44

45 MODEL DIODA DENGAN rD

46 DIODA TANPA rD

47 DIODA TANPA rD

48 1 2 3

49 POWER SUPPLY CATU DAYA

50

51 PENYEARAH GELOMBANG PENUH

52 TRAFO TANPA CENTER TAP (PENYEARAH BRIDGE)

53 FILTER C

54 PENGARUH BEBAN RL

55 RIPLE (RIAK)

56 SUPERDIODA (PENYEARAH PRESISI)

57 CLIPPER (PEMANGKAS) Vout Vin D1 D2 L+ L- Vin : tegangan sinus

58 PR Vin adalah tegangan kotak ± 10 Volt

59 PENGGESER DAN PENGARUH R

60 PENGGANDA TEGANGAN TEGANGAN PADA D1

61 PENGHASIL TEGANGAN GANDA (DUAL SUPPLY)