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Maximum Power Transfer with Negative Thevenin Resistance? |
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| Sep11-12, 05:58 PM | #1 |
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Maximum Power Transfer with Negative Thevenin Resistance?
Hello everyone! I have a general question about how to find out the maximum power transfer to a load resistor with a negative Thevenin Resistance (Rth < 0). I know for positive cases, P = R*(Vth/(R + Rth))^2, in which R is the load resistor connected to the Thevenin equivalence circuit, and Pmax = (Vth)^2/(4*Rth). But what if Rth < 0? I don't think that the Pmax equation still holds true in negative cases for Rth. Can someone help me explain this phenomenon please? I very much appreciate your help! Thank you.
Sincerely, gta100 |
| Sep11-12, 06:19 PM | #2 |
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What is a negative Thevenin resistance? Is it physical? Or is it related to some complex impedance (in which case there is a good answer)? |
| Sep11-12, 06:28 PM | #3 |
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Hello berkeman! Thank you very much for your reply!
By negative Thevenin resistance, I mean Rth < 0 in the Thevenin equivalent circuit. According to my textbook, negative Rth may appear when there are ONLY DEPENDENT sources inside "the circuit". By "the circuit", I mean the circuitry with CONSTANT PHYSICAL QUANTITIES FOR ALL ELEMENTS and with two terminals connected to a load resistor with a VARYING RESISTANCE (rheostat). I hope that is clear? Thank you! gta100 |
| Sep11-12, 06:59 PM | #4 |
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Maximum Power Transfer with Negative Thevenin Resistance?Can you post a typical circuit that exhibits negative resistance at its two output terminals? And then see if you might be able to answer your own question by trying some different resistances connected to those terminals? |
| Sep11-12, 07:26 PM | #5 |
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So in this circuit, I find Rth = -15000/11 ohms = - 1363.636364 ohms , and Vth = - 2680/11 V (Also negative). I need to find the maximum power transfer to the rheostat R as indicated. Thank you for your help! gta100 |
| Sep11-12, 08:54 PM | #6 |
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Forgetting Thevenin equivalent reistance for a moment, have you determined i(R) for arbitrary R?
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| Sep11-12, 09:01 PM | #7 |
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Hello rude man! Thank you for your reply.
I have determined i(R) for sure. It is Vth/(R + Rth), right? I actually included it in the formula for the power transferred to the load resistor, namely, P = R*(Vth/(R + Rth))^2. I even plotted the equation in MATLAB, and it turned out that P will reach infinitely high when R = - Rth (Recall that Rth < 0 now, so R = -Rth > 0). So it seems like there is no max power. Could you help me investigate if I calculated the wrong Rth? I attached the sample problem in my last post. Thank you very much! gta100 |
| Sep12-12, 12:29 AM | #8 |
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gta100,
I solved this problem using node analysis, as shown in the attachment. I don't see Thevenin helping very much. Check my node calculations. I show that when R=1363.636364, then the power dissipated in R is 2.962740001E21, a very large number. Included is a plot of the power dissipated. Ratch |
| Sep12-12, 03:35 AM | #9 |
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)Yes the maximum power is unlimited (infinity if you like), as R_L approaches -R_thv. The direction that Berkeman was trying to point you toward was to consider what type of real circuit components can produce a negative resistance. When you do this you'll find that in all cases the negative resistance is a result of some active component that is only valid over a limited operating range. There is no such thing as a true (or intrinsic) negative resistance. Common examples of negative resistances are. 1. Small signal linearized examples like the tunnel diode, where both V and I are actually in the same direction, but [itex]dV/dI[/itex] is negative over some limited range of its V/I characteristics. 2. Active circuits using opamps and transistors. (remember that these always have a limited linear operating range). 3. Electro-mechanical systems like motors and generators. Again these will always be subject to a finite operating range. |
| Sep12-12, 08:33 AM | #10 |
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Hello uart! Thank you very much for your reply! That is very inspirational and reassuring! Thank you for quoting some real-world examples which would produce negative Thevenin resistances!
gta100 |
| Sep12-12, 10:01 AM | #11 |
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uart,
Ratch |
| Sep12-12, 10:19 AM | #12 |
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For any circuit that has a negative Thevenins resistance (and a non zero Thevenins voltage) it is easy to see that if you make the external resistance equal to the absolute value of the Thevenins resistance that the total resistance becomes zero. The current, and therefore the load power, must be infinite. As I explained to gta100 however, in reality this can never happen, as the active components forming the negative resistance will limit or saturate at some finite level. |
| Sep12-12, 10:34 AM | #13 |
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uart,
Ratch |
| Sep12-12, 10:53 AM | #14 |
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Recognitions:
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| Sep12-12, 11:55 AM | #15 |
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uart,
Ratch |
| Sep12-12, 12:04 PM | #16 |
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Recognitions:
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| Sep12-12, 12:21 PM | #17 |
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[tex]\frac{2.173 R}{(0.00605R - 8.25)^2}[/tex] increases without bound as R approaches [itex]\frac{8.25}{0.00605}[/itex]? * Equation taken from your own working (with factor of [itex]10^{24}[/itex] removed top and bottom). |
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| power transfer, thevenin, thevenin equivalent, thevenin theorem, thevenin's theorem |
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