Kuliah elektronika dasar minggu ke 4 dioda
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Kuliah Elektronika Dasar Minggu ke 4 DIODA. Jurusan Teknik Elektro Fakultas Teknik UGM 2007. +. -. -. +. FUNCTION. Electrical ‘gate’ Current only flows one way Forward biased Current flows Reverse biased Blocks current. I-V characteristic. Forward Bias. Breakdown Voltage.

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Kuliah Elektronika Dasar Minggu ke 4 DIODA

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Kuliah elektronika dasar minggu ke 4 dioda

Kuliah Elektronika Dasar Minggu ke 4DIODA

Jurusan Teknik Elektro

Fakultas Teknik UGM

2007


Kuliah elektronika dasar minggu ke 4 dioda

+

-

-

+

FUNCTION

  • Electrical ‘gate’

    • Current only flows one way

  • Forward biased

    • Current flows

  • Reverse biased

    • Blocks current


Kuliah elektronika dasar minggu ke 4 dioda

I-V characteristic

Forward Bias

Breakdown Voltage

Reverse saturation current

0.7V Switch-on

Reverse Bias


Kuliah elektronika dasar minggu ke 4 dioda

PN CONSTRUCTION

  • Semiconductor material

  • n-type

    • Excess electrons

  • p-type

    • Excess holes

  • ‘Join’ together

    • Depletion region

    • Redistribution of charge carriers

    • Contact potential

      • 0.7V


Kuliah elektronika dasar minggu ke 4 dioda

SAMBUNGAN PN

  • p-type material

  • n-typematerial

  • Holesdiffuse into the n-type and ‘swallow’ electrons

  • Electronsdiffuse into the p-type and ‘fill holes’

  • Depletion region formed

    • No free charge carriers

    • 0.7V contact potential


Kuliah elektronika dasar minggu ke 4 dioda

V> 0.7V

+

+

P

N

FORWARD BIAS

  • Applied voltage above 0.7V

    • depletion region is removed

    • charge carriers can flow

  • Depletion region narrows as applied voltage approaches 0.7V

V< 0.7V

Depletion Region

DAERAH DEPLESI MENYEMPIT  MENGHILANG


Kuliah elektronika dasar minggu ke 4 dioda

V< 0V

V<< 0V

REVERSE BIAS

  • Depletion region extends

  • Higher voltage

    • Breakdown

    • Current flow

+

+

DAERAH DEPLESI MELEBAR  MAKIN LEBAR


Kuliah elektronika dasar minggu ke 4 dioda

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.


Kuliah elektronika dasar minggu ke 4 dioda

PITA ENERGI SEBUAH ATOM

PITA HANTARAN

CELAH ENERGI

PITA VALENSI

INTI


Kuliah elektronika dasar minggu ke 4 dioda

PITA ENERGI

PITA HANTARAN

No Gap

PITA HANTARAN

Large Gap

PITA HANTARAN

Small Gap

PITA VALENSI

PITA VALENSI

PITA VALENSI

Insulators

Metals

Semiconductors


Kuliah elektronika dasar minggu ke 4 dioda

Elektron di orbit terluar

Silicon

Tetravalent

Boron

Trivalent

“Acceptor”

Phosphorus

Pentavalent

“Donor”


Kuliah elektronika dasar minggu ke 4 dioda

PITA ENERGI

PITA HANTARAN

celah energi

PITA VALENSI

elektron


Kuliah elektronika dasar minggu ke 4 dioda

TERBENTUKNYA HOLE

PITA HANTARAN

ELEKTRONBEBAS

ENERGI

TAMBAHAN

elektron

PITA VALENSI

HOLE

Jumlah Elektron Bebas = Jumlah Hole


Kuliah elektronika dasar minggu ke 4 dioda

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.


Kuliah elektronika dasar minggu ke 4 dioda

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


Kuliah elektronika dasar minggu ke 4 dioda

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


Kuliah elektronika dasar minggu ke 4 dioda

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


Kuliah elektronika dasar minggu ke 4 dioda

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.


Kuliah elektronika dasar minggu ke 4 dioda

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


Kuliah elektronika dasar minggu ke 4 dioda

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


Kuliah elektronika dasar minggu ke 4 dioda

p

n

Diode current – voltage (I-V) characteristics

Semiconductor diode consists of a p-n junction with two contacts attached to the p- and n- sides

V

0

IS is usually a very small current, IS≈ 10-17 …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.


Kuliah elektronika dasar minggu ke 4 dioda

Δίοδος


Kuliah elektronika dasar minggu ke 4 dioda

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.


Ikatan kovalent

IKATAN KOVALENT


Silikon dipanasi

SILIKON DIPANASI


Di doping atom bervalensi 5

DI DOPING ATOM BERVALENSI 5

BAHAN

N

ION POS


Di doping atom bervalensi 3

DI DOPING ATOM BERVALENSI 3

BAHAN

  • P

ION NEG


Di doping atom bervalensi 51

DI DOPING ATOM BERVALENSI 5

BAHAN

N

ION POS


Di doping atom bervalensi 31

DI DOPING ATOM BERVALENSI 3

BAHAN

  • P

ION NEG


Bagaimana membuat bahan n

BAGAIMANA MEMBUAT BAHAN N ?

  • Bahan silikon diberi doping atom bervalensi 5

    • (misal : pospor)

Atom pospor disebut DONOR

Uap pospor

N

Si

RUANG HAMPA


Kuliah elektronika dasar minggu ke 4 dioda

Bahan semikonduktor jenis P

  • Bahan silikon diberi doping atom bervalensi 3

    • (misal : boron)

Atom boron disebut ASEPTOR

Uap boron

P

Si

RUANG HAMPA


Distribusi hole

DISTRIBUSI HOLE


Tegangan kontak

TEGANGAN KONTAK


Kuliah elektronika dasar minggu ke 4 dioda

Simbul dioda dan arah arus

Karakteristik ideal

Rangkaian ekivalen saat forward bias

Rangkaian ekivalen saat reverse bias


Pendekatan ideal

PENDEKATAN IDEAL


Kuliah elektronika dasar minggu ke 4 dioda

p- n diode applications:

current rectifiers

+

-

+

-

Voltage

Current

Time

Time


Penyearah setengah gelombang

PENYEARAH setengah gelombang

Tegangan input

Saat forward

π

0

Tegangan output

Saat reverse


Tegangan dc rata rata

TEGANGAN DC RATA-RATA

  • Mengintegralkan satu periode

VDC


Bila ada tegangan lawan

Bila ada tegangan lawan


Contoh rangkaian dioda

Contoh rangkaian dioda


Melihat detil

MELIHAT DETIL


Pengaruh panas

PENGARUH PANAS


Garis kerja load line

GARIS KERJA (load line)


Model dioda dengan r d

MODEL DIODA DENGAN rD


Dioda tanpa r d

DIODA TANPA rD


Dioda tanpa r d1

DIODA TANPA rD


Kuliah elektronika dasar minggu ke 4 dioda

2

3

1


Power supply catu daya

POWER SUPPLYCATU DAYA


Penyearah gelombang penuh

PENYEARAH GELOMBANG PENUH


Trafo tanpa center tap penyearah bridge

TRAFO TANPA CENTER TAP(PENYEARAH BRIDGE)


Filter c

FILTER C


Pengaruh beban r l

PENGARUH BEBAN RL


Riple riak

RIPLE (RIAK)


Superdioda penyearah presisi

SUPERDIODA (PENYEARAH PRESISI)


Clipper pemangkas

D1

Vin

D2

Vout

L+

L-

CLIPPER (PEMANGKAS)

Vin: tegangan sinus


Kuliah elektronika dasar minggu ke 4 dioda

PR

Vin adalah tegangan kotak ± 10 Volt


Penggeser dan pengaruh r

PENGGESER DAN PENGARUH R


Pengganda tegangan

PENGGANDA TEGANGAN

TEGANGAN PADA D1


Penghasil tegangan ganda dual supply

PENGHASIL TEGANGAN GANDA(DUAL SUPPLY)


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