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2 common base BJT amplifier projects

The common base is little known configuration for amplifiers using BJT. This type is used in high frequencies.

Link to the post about BJT’s operation.

BJT operationClick here

Common base amplifier with NPN transistor

common base circuit

First, the transistor must be defined, in this project was used the BC548, which has many datasheets that can be found in this link. The supply voltage (VCC) was arbitrarily chosen as 15V. While input impedance, which must have a low value, was considered as 50Ω.

Defining emitter and collector resistors

The value of resistance on emitter (Re) was chosen as 2.2kΩ. Below is the equation of input impedance for common base amplifiers.

Zi=RereRe+reZi=\frac{Re\cdot r_{e}}{Re+r_{e}}

50=2200re2200+re50=\frac{2200\cdot r_{e}}{2200+r_{e}}

re=51.1Ωr_{e}=51.1\Omega

Finding the current emitter value.

re=VTIEr_{e}=\frac{V_{T}}{I_{E}}

IE=26m51,1=0.508mAI_{E}=\frac{26m}{51,1}=0.508mA

Calculating emitter (VEV_{E}) and base (VBV_{B}) voltages. Knowing that base-emitter voltage (VBEV_{BE}) is 0.7V.

VE=ReIE=22k0.508m=1.1176VV_{E}=Re\cdot I_{E}=22k\cdot 0.508m=1.1176V

VBE=VBVEV_{BE}=V_{B}-V_{E}

VB=1.876VV_{B}=1.876V

Collector voltage value (VCV_{C}) is arbitrary. However, it must be higher than VBV_{B}, otherwise the circuit won’t amplify the signal. As was explained in the first part of BJT polarization. I choose VCV_{C} as 7.5V, half of VCC. The collector current (ICI_{C}) and emitter current (IEI_{E}) can be considered as equal.

IEIC=0,508mAI_{E}\simeq I_{C}=0,508mA

Rc=VCCVCIC=14.76kΩRc=\frac{VCC-V_{C}}{I_{C}}=14.76k\Omega

The closest commercial value is 15kΩ. In common base, output impedance (ZoZ_{o}) has the same value of Rc.

Defining base resistors

Using voltage divider equation.

VB=Rb2VCCRb2+Rb1V_{B}=\frac{Rb2\cdot VCC}{Rb2+Rb1}

1.876=Rb215Rb2+Rb11.876=\frac{Rb2\cdot 15}{Rb2+Rb1}

Rb1=6.996Rb2Rb1=6.996\cdot Rb2

Considering Rb2 as 1kΩ, Rb2 is equal to 6.996kΩ. The closest commercial available value is 8.2kΩ.

Calculating capacitors

Equation to calculate input capacitor value.

f=12πCiZif=\frac{1}{2\pi \cdot Ci\cdot Zi}

Input impedance ZiZi is 50Ω and frequency arbitrary value is 100kHz.

Ci=12πfZi=12π10550=31,83nFCi=\frac{1}{2\pi fZi}=\frac{1}{2\pi \cdot 10^{5}\cdot 50}=31,83nF

The closest commercial available value is 47nF, which gives a cutoff frequency of 67.7kHz. Can also use one of 33nF. Designing output capacitor, where output impedance (ZoZo) is 15kΩ.

Co=12πfZo=12π10515000=106pFCo=\frac{1}{2\pi fZo}=\frac{1}{2\pi \cdot 10^{5}\cdot 15000}=106pF

The commercial value is 100pF. Calculating bypass capacitor Cb, cutoff frequency was arbitrarily chosen as 500kHz.

Cb=12πfRb2=12π5105103=318pFCb=\frac{1}{2\pi fRb2}=\frac{1}{2\pi \cdot 5\cdot 10^{5}\cdot 10^{3}}=318pF

The commercial value is 270pF, which gives a cut frequency of 589.4kHz.

common base BJT amplifier complete

Common base amplifier with PNP transistor

PNP common base amplifier

The used BJT is BC558, whose datasheets are on this link. Input impedance (Zi) is 50Ω again and supply voltage is -20V.

Calculating resistors

Re was chosen as 1.8kΩ.

Zi=RereRe+reZi=\frac{Re\cdot r_{e}}{Re+r_{e}}

50=1800re1800+re50=\frac{1800\cdot r_{e}}{1800+r_{e}}

re=51.4Ωr_{e}=51.4\Omega

Finding collector current. With PNP transistor, it has a negative value.

re=VTIEr_{e}=\frac{V_{T}}{\left| I_{E}\right|}

IE=26m51.4=0.506mA\left| I_{E}\right|=\frac{26m}{51.4}=0.506mA

Calculating voltages on BC558’s terminals. Since transistor is PNP, voltages must be negative.

VE=ReIE=0.9108VV_{E}=Re\cdot I_{E}=-0.9108V

VBE=VBVEV_{BE}=V_{B}-V_{E}

0.7=VB+0.9108-0.7=V_{B}+0.9108

VB=1.6108VV_{B}=-1.6108V VCV_{C} value is arbitrarily, but it must be lower than VBV_{B}, because it’s a PNP amplifier. VCV_{C} is equal to -10V, half of supply voltage. Calculating collector resistance.

Rc=VDCVCICRc=\frac{VDC-V_{C}}{I_{C}}

IEIC=0.506mAI_{E}\simeq I_{C}=-0.506mA

Rc=20+100.506m=19.7kΩRc=\frac{-20+10}{-0.506m}=19.7k\Omega

Commercial value of Rc is 22kΩ and it’s equal to output impedance Zo. Calculating base resistors.

VB=Rb2VCDRb2+Rb1V_{B}=\frac{Rb2\cdot VCD}{Rb2+Rb1}

1.6108=20Rb2Rb2+Rb1-1.6108=\frac{-20\cdot Rb2}{Rb2+Rb1}

1.6108Rb1=18.3892Rb2-1.6108\cdot Rb1=-18.3892\cdot Rb2

Arbitrary value: Rb2=1kΩ.

Rb1=11.41kΩRb1=11.41k\Omega

Rb1 commercial value is 12kΩ.

Calculating capacitors

Defining input capacitor (Ci) arbitrarily as 10nF and calculating cutoff frequency f.

f=12πCiZi=12π10850=318.3kHzf=\frac{1}{2\pi \cdot Ci\cdot Zi}=\frac{1}{2\pi \cdot 10^{-8}\cdot 50}=318.3kHz

Calculating output capacitor Co.

f=12πCoZof=\frac{1}{2\pi \cdot Co\cdot Zo}

Co=12π318.310322103=22.7pFCo=\frac{1}{2\pi \cdot 318.3\cdot 10^{3}\cdot 22\cdot 10^{3}}=22.7pF

The commercial value is 22pF. Designing the bypass capacitor Cb, cutoff frequency is 1MHz.

Cb=12πfRb2=12π106103=159pFCb=\frac{1}{2\pi f\cdot Rb2}=\frac{1}{2\pi \cdot 10^{6}\cdot 10^{3}}=159pF

Cb commercial value is 150pF. The complete amplifier below.

PNP common base amplifier

Common base amplifiers’ video

The common base amplifier must receive a signal with very low amplitude, otherwise the output signal will be saturated and will have a different shape from input signal. Blue=input and yellow=output.

About Pedro Ney Stroski

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