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What kind of op-amp is that? |
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| Mar3-12, 02:51 AM | #52 |
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What kind of op-amp is that?If the output goes up when the input goes up, that's a non-inverting configuration. It has nothing to do with the direction of current at the input or output. |
| Mar3-12, 09:34 PM | #53 |
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Femme_physics, I notice in your calculation of V(-) you used an erroneous formula for the resistive divider involving Rb:
![]() So Rb and Rx will need to be recomputed. Circuit parameters do evaluate to nice round figures now. "... so I think you should return the flowers..."
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| Mar5-12, 12:46 AM | #54 |
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| Mar5-12, 01:09 AM | #55 |
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The circuit is also definitely an inverting amplifier, gain = -1.4 v/v. Using the lower end of R1 for input, if you change the input voltage from 0v (ground) to -0.5v, the output rises from +12v to +12.7v. Viewed this way, the zener functions to bias the op-amp so as to allow operation from a single polarity power supply. |
| Mar5-12, 03:26 AM | #56 |
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Q-Fever....OK, this is an attempt to see if the working point at V+=V-=Vout=0V is stable.
Note that my knowledge about electronics is very limited and that this may be a completely wrong way of looking at the problem. Let's assume the following: The op-amp as a huge open-loop gain G such that Vout=G(V+ - V-) + Vs/2. G will be something like 10^4 or 10^6. Vs/2 is the midpoint between the supply and ground. Looking at the characterstic curve of the Zener diode: Around 0V, the Zener diode behaves like a resistor with a fairly large impedance Rz. I guess Rz>RI/4 (you will see later why). Let's say Rz=6.5 kΩ just to have a number. Now assume V+=ε, a small voltage and V-=0 (it works the same way with V=-ε or V+=ε1 and V-=ε2). You then get Vout = G ε + Vs/2, which leads to V-=RI/(Rb+RI)*(Gε+Vs/2)=0.42 (Gε+Vs/2) V+=Rz/(Ra+Rz)*(Gε+Vs/2)=0.65(Gε+Vs/2) V+ - V- = (0.65-0.42)(Gε +Vs/2) which is larger than the starting point (which was ε), so the situation is unstable and Vout will drift up until the Zener no longer behaves as a resistor. For a very small value of ε the constant offset Vs/2 on the output voltage dominates. It does not even matter if ε is positive or negative For this to be the case RI cannot be too large, RI < Rb/Ra Rz. For those who wonder if the assumption Vout=G(V+ - V-) + Vs/2 is compatible with the "normal" operation of the circuit: Assume V+=5V and V-=5v-ε, Vout=12V and G=10000. Then you get G(5V - (5V-ε))+Vs/2 = Gε + 12.5V = 12V, i.e. ε=-0.5V/G=-50μV which can be neglected. At the operating point with Vz=5V, the Zener diode has a very steep characteristic curve, i.e. a very small impedance. If Vout changes, the change in V+ will be much smaller than that in V-, so that the negative feedback dominates and Vout is stabilized. So, NascentOxygen, am I thinking along the right lines here? (I've just made it up, don't be too polite if it's all BS). |
| Mar8-12, 06:33 AM | #57 |
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You analysis is spot on. Below the zener breakdown, the amplifier has more positive feedback than negative. This could send Vout towards 0 but nothing happens that would keep it there, and any noise that sends Vout towards +Vs will succeed, owing to a nett positive feedback. Well done! |
| Mar8-12, 06:57 AM | #58 |
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Thanks for checking.
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