I am calculating the voltage output of the below circuit. The output I have calculated varies by 0.1 of a volt compared with the simulation I created using multisim, but I am not certain this is correct.
The questions I have:
- Are the below calculations correct?
- How do I display the results in decibels
- What is the ouput voltage with no load?
Thank You.
Values:
$$Vs=70mV_{peak}$$
$$2n9304\beta = 100$$
DC Analysis:
$$V_B=Vcc.(R2/(R2+R1))=1.689V $$
$$V_E=V_B-0.7V=0.989V$$
$$I_E=(V_E/(R4+R5))=0.899mA$$
$$V_C=VCC.(IC*R3)=3.022V$$
$$RE=(V_T/I_E)=(23mV/0.899mA)=25.584\Omega$$
AC Analysis (Voltage Gain):
$$Av_{no load}=V_{out}/V_{in}=((R3*IC)/((RE+R4)*IE)=(2.2k\Omega/125.584)=17.518 $$
$$Z_{in}=(R1||R2)||(Z_{INQ})$$
$$Z_{INQ}=V_{in}/I_{in}=(125.584*I_E)/I_B=12683.984\Omega$$
$$Z_{in}=2667.24$$
$$OutputVoltage=V_s*(Z_{in}/(Z_{in}*Rs)*Av_{no load}*(RL/(RL+R3)$$
$$OutputVoltage=0.929_p=1.857_{p-p}$$
Best Answer
You know, for the base resistor divider pair, that \$V_\text{TH}=V_1\frac{R_2}{R_1+R_2}\$ and that \$R_\text{TH}=\frac{R_1\,\cdot\, R_2}{R_1+R_2}\$. From this, KVL yields:
$$V_\text{TH}-R_\text{TH}\cdot I_\text{B}-V_\text{BE}-\left(\beta+1\right)I_\text{B}\cdot\left(R_4+R_5\right)=0\:\text{V}$$
Solving the above for \$I_\text{B}\$ (unless you say otherwise, I'll assume you can plug in values and compute it) you can then find that:
$$V_\text{B}=V_\text{TH}-R_\text{TH}\cdot I_\text{B}$$
The value you get from the above is not \$V_\text{B}\approx 1.689\:\text{V}\$. It is more like \$V_\text{B}\approx 1.658\:\text{V}\$, taking your assumption \$V_\text{BE}=700\:\text{mV}\$ and \$\beta=100\$. (That's only a \$30\:\text{mV}\$ difference. But since we are calculating values using formulas, we should arrive at the same figure.) So \$V_\text{E}\approx 0.958\:\text{V}\$ and \$I_\text{E}\approx 871\:\mu\text{A}\$. So \$r_e\approx 29.86\:\Omega\$.
So far, though, we haven't considered the input signal attenuation. Before going further, it might be a good time to go back and do that. With your input capacitance at \$1\:\mu\text{F}\$ and \$f=1\:\text{kHz}\$, I find \$X_{\text{C}_1}\approx 159.2\:\Omega\$. \$C_1\$ and \$R_\text{S}\$ are in quadrature to each other, so the source impedance works out to about \$272\:\Omega\$. The load seen by your source will come from the base divider pair and the BJT's base load, or \$R_\text{IN}=R_1\mid\mid R_2\mid\mid \left(\beta+1\right)\cdot R_4\$. This is about \$2.525\:\text{k}\Omega\$ and it suggests that the input will be attenuated down to about 90% of the source magnitude. This needs to be accounted for in your estimate of the total gain.
Discounting any load and also the Early Effect, this means \$\mid\, A_v\mid \approx 90\%\frac{R_3}{R_4+r_e}\frac{\beta}{\beta+1}\approx 15.1\$. If you now add in the \$10\:\text{k}\Omega\$ load, the output is attenuated to another \$\approx \frac{10\:\text{k}\Omega}{10\:\text{k}\Omega+2.2\:\text{k}\Omega}\approx 82\%\$, or down to \$\mid\, A_v\mid \approx 12.4\$.
I'm holding short of providing detailed answers to every nuance in your questions, for now. I think you can work with what I've provided here to reach them on your own. However, one note. You should be able to find, literally everywhere on the web, the formula for decibels given a voltage ratio: \$20\log_{10} \mid\frac{v_{out}}{v_{in}}\mid\,=20\log_{10} \mid A_v\,\mid\$. You should be able to easily calculate that value for both unloaded and loaded cases.