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Dr. Khalid Al-Hindi

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(1)

Dr. Khalid Al-Hindi

(2)

N-type and P-type Materials

Proprieties

(3)

لاؤس : رثكلاا لقانلا وه ام ةداملا يف لقلاا لقانلاو

n-type material

؟

باوج :

رثكلاا لقانلا majority carrier

electrons وه

لقلاا لقانلاو minority carriers

holes وه

يلاتلا لكشلا رظنا

3

In n-type semiconductors, electrons are the majority carriers and holes are the minority carriers.

(4)

لاؤس : ةدام ةيمست ببس ام n-type material

؟ مسلاا اذهب

باوج :

رثكلاا لقانلا نلا ببسلا majority carrier

وه اهيف electrons

ةبلاس ةنحش لمحي وهو negative

يلاتلا لكشلا رظنا

4

The term n-type comes from the negative charge of the electron.

(5)

لاؤس : رثكلاا لقانلا وه ام ةداملا يف لقلاا لقانلاو

p-type material

؟

باوج :

رثكلاا لقانلا majority carrier

holes وه لقلاا لقانلاو

minority carriers electrons وه

يلاتلا لكشلا رظنا

5

In p-type semiconductors, holes are the majority carriers and electrons are the minority carriers.

(6)

لاؤس : ةدام ةيمست ببس ام p-type material

؟ مسلاا اذهب

باوج :

رثكلاا لقانلا نلا ببسلا majority carrier

وه اهيف holes

ةبجوم ةنحش لمحي وهو positive

رظنا

يلاتلا لكشلا

6

The term p-type comes from the positive charge of the holes.

(7)

P-N Junction

(8)

لاؤس : نيتداملا عنص نم ةدئافلا يه ام n-type material

و p-type material

؟

باوج :

يلاتلا لكشلا رظنا ةفلتخملا ةينورتكللاا ةزهجلاا ةعانص يف نيتيساسلاا نيتداملا امهنلا

8

The n-type and p-type materials represent the basic building blocks of semiconductor devices.

(9)

لاؤس : نيتداملا نم ةدافتسلاا متي فيك n-type material

و p-type material

؟

باوج :

ب فرعي ام نيوكتو امهضعب راوجب نيتداملا ةعانصب كلذ متي p-n junction

يلاتلا لكشلا رظنا

9

Joining of a single n-type material with a p-type material will result in a semiconductor element of considerable importance in electronic systems.

(10)

لاؤس : وه ام p-n junction

؟

باوج :

يلاتلا لكشلا رظنا ضعبلا امهضعب راوجب نيتداملا عضوب هتعانص متي زاهج وه

10

A p-n junction is created by simply joining an n-type and a p-type material together, nothing more, just the joining of one material with a majority carrier of electrons to one with a majority carrier of holes.

(11)

لاؤس : دوجو ىلع دامتعلااب ةعونصملا ةينورتكللاا ةزهجلاا رهشا يه ام p-n junction

؟

باوج :

يلاتلا لكشلا يف نيحضوم مهرهشا

11

Transistor

JFET Diode

(12)

P-N Junction Physics

(13)

لاؤس : عنص دعب ةرشابم ثدحي اذام p-n junction

؟

باوج :

ىمست ةيطسو ةقطنم نوكتت ايئاقلت depletion region

يلاتلا لكشلا رظنا

13

When a p-n junction is formed, a depletion region occurs.

(14)

لاؤس : ةقطنم يه ام depletion region

؟

باوج :

يف ءاقتللاا ةقطنم يه p-n junction

تانحش لمحتو ايعيبط ثدحتو لكشلا رظنا ةبلاسو ةبجوم ions

يلاتلا

14

A region in a semiconductor device at the juncture of P-type and N-type materials, in which there is neither an excess of electrons nor of holes.

(15)

لاؤس : ةقطنم ثودح ببس وه ام depletion region

؟

باوج :

نم ةرحلا تانورتكللاا كرحت وه اهثودح ببس n-type

عم دحتتل holes

يف ةدوجوملا p-type

ةثدحم

تانحش ةقطنم يف ions

depletion region يلاتلا لكشلا رظنا

15

When a p-n junction is formed, some of the free electrons in the n-region diffuse across the junction and combine with holes to form negative ions. In so doing they leave behind positive ions at the donor impurity sites.

(16)

P-N Junction Diode

(17)

لاؤس : وه ام زاهجل يلخادلا بيكرتلا

Diode

؟

باوج :

زاهجل يلخادلا بيكرتلا Diode

نع ةرابع وه p-n junction

يلاتلا لكشلا رظنا

17

The semiconductor diode is a p-n junction.

(18)

لاؤس : زاهج فارطا ىمست اذام Diode

؟

باوج :

ىمست anode

cathode و يلاتلا لكشلا رظنا

18

Anode and cathode diode terminals.

(19)

لاؤس : زاهج لخاد ثدحي اذام Diode

؟ ءابرهكلاب هليصوت مدع نيح

باوج :

يلاتلا لكشلا رظنا رايت يا هب رمي لاو ءيش ثدحيلا

19

When the applied voltage is 0 V (no bias), then the resulting current is 0 A, much like an isolated resistor.

(20)

لاؤس : زاهج لخاد ثدحي اذام Diode

عضو يف نوكي امنيح Reverse-Bias

؟

باوج :

ةقطنم ضرع دادزي depletion region

رظنا رايتلا رورم عنمت يتلاو يلاتلا لكشلا

20 If an external potential of V volts is

applied across the p–n junction such that the positive terminal is connected to the n-type material and the negative terminal is connected to the p-type material as shown in Fig. 1.13 , the number of

uncovered positive ions in the depletion region of the n-type material will increase due to the large number of free electrons drawn to the positive potential of the applied voltage. For similar reasons, the number of uncovered negative ions will increase in the p-type material. The net effect, therefore, is a widening of the depletion region. This widening of the depletion region will establish too great a barrier for the majority carriers to

overcome, effectively reducing the

majority carrier flow to zero, as shown in Fig. 1.13a .

(21)

لاؤس : زاهج لخاد ثدحي اذام Diode

عضو يف نوكي امنيح Forward-Bias

؟

باوج :

ةقطنم شمكنت depletion region

للاخ رايتلا رميو diode

رظنا لكشلا يلاتلا

21 As the applied bias increases in magnitude, the depletion region will continue to decrease in width until a flood of electrons can pass through the junction, resulting in an exponential rise in current as shown in the forward- bias region of the characteristics of Fig. 1.15 . Note that the vertical scale of Fig. 1.15 is measured in milli-

amperes (although some semiconductor diodes have a vertical scale measured in amperes), and the horizontal scale in the forward-bias region has a maximum of 1 V.

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