EDC - BJT
.HISTORY.                                                           .Construc�on.
                                                                       The BJT is constructed with three doped semiconductor regions
1904 - J.A Fleming                                                      separated by two P -N junc�ons.
    Vacuum Tube Diode
                                                                       The term bipolar refers to the use of both holes and electrons
     AKA Fleming Valve, Thermionic Valve
                                                                        as current carriers in the transistor structure.
    Thermionic Emission
                                                                    Base – Emiter (BE) Junc�on
                                                                       The PN junc�on joining the base region and the emiter region.
                                                                    Base – Collector (BC) Junc�on
                                                                       The PN junc�on joining the base region and the collector
                                                                        region.
1906 - Lee de Forest                                                Width:            1. Collector
    Vacuum Tube Triode                                                               2. Emiter
    Added a 3rd element to the vacuum tube                                           3. Base               Base – Width Ra�o(1:150)
     called the Control Grid.
                                                                    Doping:           1. Emiter             – Heavily doped
    1st amplifier.
                                                                                      2. Collector
                                                                                      3. Base               – lightly doped
                                                                                                        Majority Carrier: Electron
                                                                                                         Electrons are faster.
1939 - Russell Ohl
    P-N junc�on
                                                                                                     Majority Carrier: Holes
1947 - John Bardeen
      - Water Bratain
      - William Shockley – Supervisor
    December 23, 1947
    Point Contact Transistor – 1st transistor.
                                                                    .DUAL DIODE MODEL.
1949 - William Shockley
    Bipolar Junc�on Transistor
     Bipolar – 2 carriers (electron and holes)
     Junc�on – boundary or interface between two
                   types of semiconductor materials
    Transistor – Transfer Resistor
                  - it transfers the resistance from one end
                     of the device to the other end.
                                                                                EDC - BJT
.Characteris�c Curve.                                                                     .Power Dissipa�on.
                                                                                                           𝑃𝑃𝐷𝐷 = 𝑉𝑉𝐶𝐶𝐶𝐶 ∙ 𝐼𝐼𝐶𝐶
                                                                                                                            𝑡𝑡𝑜𝑜𝑜𝑜
                                                                                                           𝑃𝑃𝐷𝐷(𝑎𝑎𝑎𝑎𝑎𝑎.) = � � 𝑉𝑉𝐶𝐶𝐶𝐶(𝑠𝑠𝑠𝑠𝑠𝑠) ∙ 𝐼𝐼𝐶𝐶(𝑠𝑠𝑠𝑠𝑠𝑠)
                                                                                                                              𝑇𝑇
                                                                                                           𝑃𝑃𝑂𝑂(𝑎𝑎𝑎𝑎) = 𝑉𝑉𝐶𝐶𝐶𝐶(𝑟𝑟𝑟𝑟𝑟𝑟) 𝐼𝐼𝐶𝐶(𝑟𝑟𝑟𝑟𝑟𝑟)
                                                                                          .Common Configura�on.
                                                                                          𝐼𝐼𝐼𝐼𝐼𝐼𝐼𝐼𝐼𝐼                                     𝐴𝐴𝐴𝐴𝐴𝐴𝐴𝐴𝐴𝐴𝐴𝐴
Cutoff Region
   Not-conduc�ng                                                                         𝐼𝐼𝐸𝐸 = 𝐼𝐼𝐵𝐵 + 𝐼𝐼𝐶𝐶                             𝐼𝐼𝐸𝐸 = 𝐼𝐼𝐵𝐵 + 𝐼𝐼𝐶𝐶 − 𝐼𝐼𝐶𝐶𝐶𝐶𝐶𝐶
   𝐼𝐼𝐶𝐶 = 0
   𝑉𝑉𝐶𝐶𝐶𝐶 ≈ 𝑂𝑂𝑂𝑂𝑂𝑂𝑂𝑂 → 𝑶𝑶𝑶𝑶𝑶𝑶𝑶𝑶𝑶𝑶                                                        𝑰𝑰𝑬𝑬 ≃ 𝑰𝑰𝑪𝑪
Ac�ve Region                                                                              𝛽𝛽 =
                                                                                                    𝐼𝐼𝐶𝐶
                                                                                                                               → 𝐶𝐶𝐶𝐶𝐶𝐶𝐶𝐶𝐶𝐶𝐶𝐶 𝐸𝐸𝐸𝐸𝐸𝐸𝐸𝐸𝐸𝐸𝐸𝐸𝐸𝐸 𝑎𝑎𝑎𝑎𝑎𝑎𝑎𝑎𝑎𝑎𝑎𝑎𝑎𝑎𝑎𝑎𝑎𝑎𝑎𝑎 𝑓𝑓𝑓𝑓𝑓𝑓𝑓𝑓𝑓𝑓𝑓𝑓, ℎ𝑓𝑓𝑓𝑓
   Conducts at normal opera�on.                                                                    𝐼𝐼𝐵𝐵
   0 < 𝐼𝐼𝐶𝐶 < 𝐼𝐼𝑠𝑠𝑠𝑠𝑠𝑠. → 𝑎𝑎𝑎𝑎𝑎𝑎 𝑎𝑎𝑎𝑎 𝑎𝑎 𝑨𝑨𝑨𝑨𝑨𝑨𝑨𝑨𝑨𝑨𝑨𝑨𝑨𝑨𝑨𝑨𝑨𝑨                                                                       𝑡𝑡𝑡𝑡𝑡𝑡𝑡𝑡𝑡𝑡𝑡𝑡𝑡𝑡𝑡𝑡𝑡𝑡 (20 − 200)𝑖𝑖𝑖𝑖 𝑛𝑛𝑛𝑛𝑛𝑛 𝑔𝑔𝑔𝑔𝑔𝑔𝑔𝑔𝑔𝑔 𝛽𝛽 = 100
                                                                                                    𝐼𝐼𝐶𝐶            𝛽𝛽
                                                                                          𝛼𝛼 =             =                  → 𝐶𝐶𝐶𝐶𝐶𝐶𝐶𝐶𝐶𝐶𝐶𝐶 𝐵𝐵𝐵𝐵𝐵𝐵𝐵𝐵 𝑎𝑎𝑎𝑎𝑎𝑎𝑎𝑎𝑎𝑎𝑎𝑎𝑎𝑎𝑎𝑎𝑎𝑎𝑎𝑎 𝑓𝑓𝑓𝑓𝑓𝑓𝑓𝑓𝑓𝑓𝑓𝑓
                                                                                                    𝐼𝐼𝐸𝐸          𝛽𝛽+1
                                                                                                    𝐼𝐼𝐸𝐸
Satura�on Region                                                                          𝛾𝛾 =
                                                                                                    𝐼𝐼𝐵𝐵
                                                                                                                               → 𝐶𝐶𝐶𝐶𝐶𝐶𝐶𝐶𝐶𝐶𝐶𝐶 𝐶𝐶𝐶𝐶𝐶𝐶𝐶𝐶𝐶𝐶𝐶𝐶𝐶𝐶𝐶𝐶𝐶𝐶 𝑎𝑎𝑎𝑎𝑎𝑎𝑎𝑎𝑎𝑎𝑎𝑎𝑎𝑎𝑎𝑎𝑎𝑎𝑎𝑎 𝑓𝑓𝑓𝑓𝑓𝑓𝑓𝑓𝑓𝑓𝑓𝑓
   Reach Max Current (𝐼𝐼𝑠𝑠𝑠𝑠𝑠𝑠. )
   𝐼𝐼𝐶𝐶 = 𝐼𝐼𝑠𝑠𝑠𝑠𝑠𝑠.                                                                                                      𝑰𝑰𝑪𝑪 = 𝜷𝜷𝑰𝑰𝑩𝑩
   𝑉𝑉𝐶𝐶𝐶𝐶 ≈ 𝑆𝑆ℎ𝑜𝑜𝑜𝑜𝑜𝑜 → 𝐴𝐴𝐴𝐴𝐴𝐴 𝑎𝑎𝑎𝑎 𝑎𝑎 𝑺𝑺𝑺𝑺𝑺𝑺𝑺𝑺𝑺𝑺𝑺𝑺
                                                                                          A BJT is a Current-Controlled Current Source (CCCS)
                                                                                          because a small change in 𝐼𝐼𝐵𝐵 can cause a large change in 𝐼𝐼𝐶𝐶 .
.Mode of Opera�on.
   Deple�on Region Shrink when FB.                                                                                      Common –                   Common –                      Common –
   Deple�on Region Widen when RB.                                                                                       Base                       Collector /                   Emiter /
                                                                                                                                                    Emiter-
         𝑅𝑅𝑅𝑅𝑅𝑅𝑅𝑅𝑅𝑅𝑅𝑅              𝐵𝐵 − 𝐸𝐸 𝐽𝐽𝐽𝐽𝐽𝐽𝐽𝐽𝐽𝐽𝐽𝐽𝐽𝐽𝐽𝐽    𝐵𝐵 − 𝐶𝐶 𝐽𝐽𝐽𝐽𝐽𝐽𝐽𝐽𝐽𝐽𝐽𝐽𝐽𝐽𝐽𝐽
𝐴𝐴𝐴𝐴𝐴𝐴𝐴𝐴𝐴𝐴𝐴𝐴                                 𝐹𝐹𝐹𝐹                        𝑹𝑹𝑹𝑹                                                                       Follower
(Amplifier)                                                                                 Applica�on                    Boltage                    Current                       Everything
𝑆𝑆𝑆𝑆𝑆𝑆𝑆𝑆𝑆𝑆𝑆𝑆𝑆𝑆𝑆𝑆𝑆𝑆𝑆𝑆                          𝐹𝐹𝐹𝐹                       𝐹𝐹𝐹𝐹                                            amplifier/                  amplifier/
(ON switch)                                                                                                                                         Isola�on/
𝐶𝐶𝐶𝐶𝐶𝐶𝐶𝐶𝐶𝐶𝐶𝐶                                  𝑅𝑅𝑅𝑅                      𝑹𝑹𝑹𝑹                                                                        Z – matching
(OFF switch)
                                                                                           Output                                  𝐼𝐼𝐶𝐶                       𝐼𝐼𝐸𝐸                          𝐼𝐼𝐶𝐶
𝑅𝑅𝑅𝑅𝑅𝑅𝑅𝑅𝑅𝑅𝑅𝑅𝑅𝑅 𝐴𝐴𝐴𝐴𝐴𝐴𝐴𝐴𝐴𝐴𝐴𝐴                   𝑅𝑅𝑅𝑅                      𝑭𝑭𝑭𝑭
                                                                                           Input                                   𝐼𝐼𝐸𝐸                       𝐼𝐼𝐵𝐵                          𝐼𝐼𝐵𝐵
                                                                                                  𝐼𝐼𝑜𝑜𝑜𝑜𝑜𝑜                    𝐼𝐼𝐶𝐶 ≃ 𝐼𝐼𝐸𝐸                𝐼𝐼𝐸𝐸 ≫ 𝐼𝐼𝐵𝐵                   𝐼𝐼𝐶𝐶 > 𝐼𝐼𝐵𝐵
                                                                                           𝑨𝑨𝒊𝒊 =
                                                                                                    𝐼𝐼𝑖𝑖𝑖𝑖                         𝐼𝐼𝐶𝐶                       𝐼𝐼𝐸𝐸                          𝐼𝐼𝐶𝐶
                                                                                                                          𝛼𝛼 = ≃ 1                    𝛾𝛾 = ≫ 1                     𝛽𝛽 = > 1
                                                                                                                                   𝐼𝐼𝐸𝐸                       𝐼𝐼𝐵𝐵                          𝐼𝐼𝐵𝐵
                                                                                                                                𝐿𝐿𝐿𝐿𝐿𝐿                     𝐻𝐻𝐻𝐻𝐻𝐻𝐻𝐻                       𝑀𝑀𝑀𝑀𝑀𝑀
.Thermal Runaway.                                                                          𝒁𝒁𝒊𝒊𝒊𝒊                               𝐿𝐿𝐿𝐿𝐿𝐿                     𝐻𝐻𝐻𝐻𝐻𝐻𝐻𝐻                       𝑀𝑀𝑀𝑀𝑀𝑀
                                                       1                                               𝑉𝑉𝑜𝑜𝑜𝑜𝑜𝑜              𝑉𝑉𝐶𝐶 ≫ 𝑉𝑉𝐸𝐸                 𝑉𝑉𝐵𝐵 ≃ 𝑉𝑉𝐸𝐸                  𝑉𝑉𝐶𝐶 > 𝑉𝑉𝐵𝐵
     𝑆𝑆𝑆𝑆𝑆𝑆𝑆𝑆𝑆𝑆𝑆𝑆𝑆𝑆 → 𝑁𝑁𝑁𝑁𝑁𝑁 �𝑇𝑇 ∝                       �                                𝑨𝑨𝒗𝒗 =
                                                       𝑅𝑅                                               𝑉𝑉𝑖𝑖𝑖𝑖                      𝑉𝑉𝐶𝐶                        𝑉𝑉𝐸𝐸                         𝑉𝑉𝐶𝐶
                                                                                                                         𝐴𝐴𝑣𝑣 =          ≫1          𝐴𝐴𝑣𝑣 =          ≃1           𝐴𝐴𝑣𝑣 =          >1
                                                                                                                                    𝑉𝑉𝐸𝐸                        𝑉𝑉𝐵𝐵                         𝑉𝑉𝐵𝐵
                                                                                                                               𝐻𝐻𝐻𝐻𝐻𝐻𝐻𝐻                     𝐿𝐿𝐿𝐿𝐿𝐿                        𝑀𝑀𝑀𝑀𝑀𝑀
                                                                                           𝒁𝒁𝒐𝒐𝒐𝒐𝒐𝒐                            𝐻𝐻𝐻𝐻𝐻𝐻𝐻𝐻                     𝐿𝐿𝐿𝐿𝐿𝐿                        𝑀𝑀𝑀𝑀𝑀𝑀
                                                                                           𝑨𝑨𝑷𝑷 = 𝐴𝐴𝑣𝑣 ∙ 𝐴𝐴𝑖𝑖                    𝑀𝑀𝑀𝑀𝑀𝑀                     𝑀𝑀𝑀𝑀𝑀𝑀                      𝐻𝐻𝐻𝐻𝐻𝐻𝐻𝐻
                                                                                           𝑃𝑃ℎ𝑎𝑎𝑎𝑎𝑎𝑎 𝑆𝑆ℎ𝑖𝑖𝑖𝑖𝑖𝑖                   𝑁𝑁/𝐴𝐴                      𝑁𝑁/𝐴𝐴                         180°
                                                               EDC - BJT
.AC Analysis.
Equivalent Circuit                                                  Frequency Response
                                                                    Low Frequency Analysis
                                                                    Cutoff-Frequency (𝒇𝒇𝑳𝑳 ) @𝑋𝑋𝐶𝐶 = 𝑅𝑅
                                                                                            1
                                                                           𝑋𝑋𝐶𝐶 = 𝑅𝑅 =
                                                                                          2𝜋𝜋𝜋𝜋𝜋𝜋
                                                                                      1
                                                                           𝑓𝑓𝐿𝐿 =
                                                                                    2𝜋𝜋𝜋𝜋𝜋𝜋
                                                                    High Frequency Analysis
                                                                                        1
                                                                           𝑓𝑓𝐻𝐻 =
                                                                                    2𝜋𝜋𝑅𝑅𝑇𝑇ℎ 𝐶𝐶
                                                                    Miller Effect Capacitance
                 ∆𝑉𝑉𝐶𝐶𝐶𝐶
       𝑟𝑟𝑜𝑜 =            ≈ ∞ ≈ 𝑜𝑜𝑜𝑜𝑜𝑜𝑜𝑜 𝑐𝑐𝑐𝑐𝑐𝑐𝑐𝑐𝑐𝑐𝑐𝑐𝑐𝑐
                  ∆𝐼𝐼𝐶𝐶
                             → 𝑢𝑢𝑢𝑢𝑢𝑢𝑢𝑢𝑢𝑢𝑢𝑢𝑢𝑢 𝑖𝑖𝑖𝑖𝑖𝑖𝑖𝑖𝑖𝑖𝑖𝑖𝑖𝑖
                 26𝑚𝑚𝑚𝑚
       𝑟𝑟𝑒𝑒 =
                   𝐼𝐼𝐸𝐸
       𝑉𝑉𝑏𝑏 = 𝐼𝐼𝑒𝑒 (𝑟𝑟𝑒𝑒 + 𝑅𝑅𝐸𝐸 )
                                                                           𝐶𝐶𝑀𝑀𝑀𝑀 = (1 − 𝐴𝐴𝑣𝑣 )𝐶𝐶𝑓𝑓
       𝑍𝑍𝑖𝑖𝑖𝑖   = 𝐵𝐵𝑎𝑎𝑎𝑎 (𝑟𝑟𝑒𝑒 + 𝑅𝑅𝐸𝐸 )
                                                                                               1
                                                                           𝐶𝐶𝑀𝑀𝑀𝑀 = �1 −          � 𝐶𝐶 ≈ 𝐶𝐶𝑓𝑓
       𝐴𝐴𝐴𝐴𝐴𝐴𝐴𝐴𝐴𝐴 → 𝑉𝑉𝑉𝑉𝑉𝑉𝑉𝑉                                                                  𝐴𝐴𝑣𝑣 𝑓𝑓
                       EDC - BJT
.Basic Configura�ons.
EDC - BJT
EDC - BJT
EDC - BJT