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| General Electronics Chat This forum is for general chat about electronics, eg: Dont know what a part does? Dont know how to read a circuit? Want to get an opinion? |
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| How would you work out the gain of the self biasing amplifier, im not sure how to begin. I was trying to use closed loop gain equations but im not sure how to apply them. Megamox EDIT: Sorry just spotted the diagram is wrong, the Resistor Rb should connect to the collector and not the rail! | |
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| You have to replace the transistor with it's small signal equivalent circuit then analyze that circuit. Also, you could use the h-parameter representation of a transistor.
__________________ see my website: www.geocities.com/russlk | |
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| The source's impedance is also part of the gain equation.
__________________ Uncle $crooge | |
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If your source has a low output resistance, then you need a different configuration.
__________________ Len | ||
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Its distortion would be so high that you would be unable to measure its gain. With a high source impedance then it wouldn't have any gain so would be an inverting piece of wire or attenuator. :wink:
__________________ Uncle $crooge | ||
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| Well i must be doing something wrong, maybe my small signal model is incorrect because im just getting massive equations with no way to seperate out the gain expression in the form of: VIN(Constant1) + Vout(Constant2) = Constant3 When it comes to transistor amplifiers, the only one it seems i can rely on to work with slightly differing hfe's, rises in temperature and leakage currents, is the fixed bias arrangement, with a resistor on the emitter and collector, but for high gains, this usually results in a high collector resistor and therefore higher output impedance, how do you guys get around this? Sometimes i add a cap on the emitter, which gives me a little extra gain but distorts the signal! Megamox | |
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| A transistor needs a high value for its collector resistor for high gain. For very high gain and fairly low distortion, transistors use a constant current source instead of a collector resistor. A constant current source has an extremely high resistance. If you need to match the high resistance to another transistor's input that has a much lower resistance then use an additional emitter-follower in between.
__________________ Uncle $crooge | |
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| This is in response to the original question. We need to qualify this discussion with the proviso that the amplifier is biased with Vc ~ Vcc/2. This is done by making Rb ~ beta*RL (not a good biasing method if you want a predictable, stable operating point). Next, let's make a couple of approximations and assumptions: 1. beta >> 1, therefore Ie ~ Ic 2. Rc >> RL where Rc is the dynamic collector resistance With these approximations, the voltage gain (with zero source resistance) is approximately -RL/re, where re~0.026/Ie. Ie is dependent on beta. So, first we have to determine the emitter current: *a bunch of equations boiling down to: (I can post these if anyone wants to see them) Ie ~ Ic = (Vcc-Vbe)/(RL+RB/beta) where Vbe~0.7 Av=-RL/re, as previously stated Solving for Av, Av=-(VCC-Vbe)/(0.026*(1+(RB/(beta*RL))) This yields low-frequency gain in the 45dB range for VCC=10V, and 100<beta<300. This gives a voltage gain for zero source impedance. As has been pointed out, high level inputs yield high distortion, and zero impedance sources are not the norm. Nevertheless, if you have a 100uV signal, distortion may be tolerable, and 50 ohm sources are common, as are emitter followers, which can have output impedances in the tens of ohms. If the source impedance Rs is high, gain will be less than Rb/Rs. | |
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| Thats great, id be interested in seeing those other equations too. Normally i use this type of amp to buffer my electret mic signals, im not sure what their typical impedances are though. | |
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(1) Vc=Vcc-Ic*RL (2) Ib*Rb=Vc-Vbe Solving (2) for Vc, (3) Vc=Ib*Rb+Vbe Rearranging (1), (4) Ic*RL=Vcc-Vc Substituting (3) for Vc in (4), (5) Ic*RL=Vcc-Ib*Rb-Vbe Rearranging (5) (6) Ic*RL+Ib*Rb=Vcc-Vbe (7) Ib=Ic/beta by definition Substitutuing (7) into (6), (8) Ic*RL*Ic*Rb/beta=Vcc-Vbe Solving (8) for Ic, (9) Ic=(Vcc-Vbe)/(RL*Rb/beta) Q.E.D. | ||
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| I measured the impedance of my electret mic. It is about 3K when it is effectively in parallel with the 10k resistor that feeds current (about 0.5mA) to it from an 8V supply. I've connected an electret mic directly (through a coupling cap) to the "virtual earth" inverting input of an opamp without a series resistor. The gain is about the same as if the opamp was non-inverting and with the same negative feedback resistor and the feedback resistor to ground the 3K resistance of the mic in parallel with the 10k resistor. It takes about 1 minute for the current of my electret mic to settle. I guess the FET in it is so small that 0.5mA heats it slowly. :lol:
__________________ Uncle $crooge | |
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| This factor 0.026, is from the diode equation right? The thermal voltage across a diode is 26mv (kt/q) at room temp. | |
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| It isn't thermal, it is the dynamic change of conductance of a semiconductor junction. When you increase the current 10 times then the voltage across the junction increases only 26mV.
__________________ Uncle $crooge | |
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Hold on! I posted a bunch of equations, and then got strange result on some of the intermediate answers. I'm re-thinking the whole thing. EDIT AGAIN: OK, I think I fingered out my mistake. This is hopefully correct: Yes, it's called the diode thermal voltage. I had to refresh my memory on the derivation: From the diode equation, I = Is*(e^(qV/kT)-1) where Is is the reverse saturation (leakage) current I/Is = e^(qV/kT)-1 I/Is ~ e^(qV/kT) for I>>Is qV/kT = ln(I/Is) V = (kT/q)*ln(I/Is) = (kT/q)*ln(I) - (kT/q)*ln(Is) dynamic resistance = dV/dI dV/dI = (kT/q)/I ; k is Boltzmann's constant, q is the charge on an electron in Coulombs, T is temperature in degrees Kelvin kT/q = .026 at T=300 Kelvin dV/dI=.026/I at T=300 Kelvin The number I remember is (26 ohms)/(current in milliamps) | ||
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| The base-emitter voltage change with temperature shows almost the same angle when the current is changed. So temperature has little effect on a transistor's Re.
__________________ Uncle $crooge | |
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