# BJT average power dissipation

Given the following circuit with $$\\beta=80\$$, $$\V_{BE(on)}=0.7V\$$, $$\V_A=\infty\$$, for an input signal $$\V_s=18cos(\omega t) mV\$$, I would like to calculate the power dissipated in the transistor. I began by calculating the thevenin equivalent voltage and resistance in order to solve for the base current as follows:

$$\R_{thev} = \frac{R_1 R_2}{R_1+R_2} = \frac{30k\Omega \times 125k\Omega}{30k\Omega + 125k\Omega} = 24.194k\Omega\$$

$$\V_{thev} = V_{cc} \frac{R_2}{R_1+R_2} = 2.32V\$$

The base current can be solved for by writing a KVL equation around the base-emitter loop and substituting $$\I_e=(\beta+1)I_b\$$:

$$\-V_{thev} + R_{thev}I_b + V_{BE(on)} + R_eIe = 0\$$

$$\-V_{thev} + R_{thev}I_b + V_{BE(on)} + R_eIb(1+\beta) = 0\$$

and solving for $$\I_b\$$:

$$\I_b = \frac{V_{thev}-V_{BE(on)}}{R_{thev} + (1+\beta)R_e} = 25.1\mu A\$$

Then $$\I_c = \beta I_b = (80)(2.006 \mu A) = 2.01mA \$$

The collector-emitter voltage can be solved for by writing the equation around the collector emitter loop:

$$\V_{CE} = V_{cc} - R_c I_c - R_e I_e = 6.973 V\$$

The power dissipated in the transistor is given by

$$\PQ = I_{CQ}V_{CEQ}-\frac{1}{2}I^2_cR_c\$$

And presumably, the power dissipated in the load is given by

$$\PL = \frac{1}{2}I^2_cR_L\$$

First I will need to solve $$\I_c\$$

I write te expression as:

$$\I_c = \beta(\frac{R_{thev}}{R_{thev} + R_{ib}})(\frac{V_s}{R_{is}})\$$

In the expression above $$\R_{ib}\$$ is the internal resistance of the transistor in the small signal model given by:

$$\R_{ib} = r_\pi + (1+\beta)R_e\$$ with $$\r_\pi = \frac{V_T}{I_b}\$$

$$\R_{is} = Rs + R_i\$$ (in this case no source resistance was indicated so it is just $$\R_i\$$)

And $$\R_i = R_{thev}||R_{ib}\$$

Therefore substituting the above expressions into $$\I_c\$$

$$\I_c = \beta(\frac{R_{thev}}{R_{thev} + r_\pi + (1+\beta)R_e })(\frac{V_s}{R_{thev}||R_{ib}})\$$

$$\ = (80)(\frac{24194}{24194+40513})(\frac{V_s}{15148}) = 1.974\times 10^{-3} V_s\$$

From this I calculate the power dissipated in the transistor to be

$$\PQ = I_{CQ}V_{CEQ}-\frac{1}{2}I^2_cR_c = (2.01mA)(6.973V) - 0.5(1.974\times 10^{-3} \times 0.018)^2(2000) = 13.98mW\$$

However the textbook answer gives $$\13.0mW\$$ rather. Where am I going wrong?

• In your last formula, did you mean for the units to come out as mA or mW? – The Photon May 8 at 14:43
• @ThePhoton my mistake, I have fixed it . – Blargian May 8 at 15:26
• Isn’t the power dissipation for a transistor simply P=Ic*Vce? – Leoman12 May 8 at 15:47
• FWIW, simulation gives 13.037mW – Spehro Pefhany May 8 at 16:19
• @Blargian but you can ignore Rth also because we know that Rs = 0Ω thus vin = vpi – G36 May 8 at 17:50

In short.

$$P_Q = I_{CQ} \times V_{CEQ} \approx 2\text{mA} \times 6.97\text{V} \approx 13.94 \text{mW}$$

And the AC component of a collector current is equal to

$$i_c = g_m v_{\pi} = 1/13\Omega \times 18 \text{mV} \approx 1.38 \text{mA}$$

Therefore power dissipated in the transistor is:

$$P_Q = I_{CQ}V_{CEQ}-\frac{i^2_c \left(R_C||R_L\right)}{2} = 13.94\text{mW} - \frac{1.38\text{mA}^2 \times 1\text{k}\Omega}{2} \approx 13\text{mW}$$

• Thank you for your answer. One thing I'm still not understanding is the distribution of power between the transistor and the load. I read that as the AC input signal increases the distribution shifts from the transistor to the load. How is the AC component of collector current distributed between the collector resistor and the load itself? – Blargian May 8 at 17:19
• @Blargian In this case, a current divider rule will do the job. $$i_{RL} = i_c \times \frac{R_C}{R_C + R_L}$$ or $$i_{R_C} = i_c \times \frac{R_L}{R_C + R_L}$$ – G36 May 8 at 17:48
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