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Here we go again! Newtons and Watts... |
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| Mar4-10, 07:59 AM | #35 |
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Here we go again! Newtons and Watts...Now assuming we are still applying the same terminal voltage to the motor when running or when it has a locked shaft what happens to the current in the armature? Where does the energy go that was being provided while running now that the shaft has been locked? Torque is still being developed on the shaft which means the electric motor is being supplied with energy. Energy cannot be destroyed, so where does the energy go? berkemen has a good point though, no machines in real life are 100% efficient so it seems a bit pointless to me to continue bringing up magical electric motors. All that I'm personally concerned with are the real motors that I deal with and how they respond. Discussions such as these have no value in the practical world for engineers. Interesting in academia though. ![]() CS |
| Mar4-10, 08:05 AM | #36 |
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Is there work being done on the Mazarati? No, because it is not moving. CS |
| Mar4-10, 04:54 PM | #37 |
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| Mar4-10, 11:44 PM | #38 |
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Unlike motors that rely on magnetic forces, electrostatic motors can, and sometimes are, designed such that their current draw is zero (or at least approximately 0) when there is no motion, while continuing to hold their force/torque. As applied to the specific application of compressing a spring and holding it in a compressed state for an extended period, the performance a properly chosen electrostatic motor can approach that of an ideal motor. |
| Mar5-10, 07:43 AM | #39 |
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One of the simplest DC machines is a loop of wire connected to a battery positioned between two permanent magnets. This is what I was referring to. As the resistance of the loop goes to zero the current would approach infinity which makes the problem indeterminate. However, if we look at the limit as the resistance goes to zero...we'll see that the current becomes really large for a given applied voltage. Since we have voltage and a large current, power is being consumed even though the shaft (loop in this case) isn't moving. The power must be dissipated as heat (some power is absorbed and stored by the magnetic field as well). CS |
| Mar5-10, 07:49 AM | #40 |
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I guess at the end of the day all we can say is that if power is being used by an electric machine that it will be converted to some other form. That form (e.g. mechanical power, heat) will depend on the device. CS |
| Mar5-10, 09:09 AM | #41 |
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| Mar5-10, 06:57 PM | #42 |
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If any of you happen to have a spare 100% efficient motor lying around, let me know. I'm willing to pay for it :-)
Anyway, I think I've gotten a bit closer to my original question conserning the relationship between Watts and Newtons. As many of you have allready explained quite detailed, there is no direct corelation between the two, BUT it seams that Amps have a very direct relation to Newtons. As mentioned several times allready: Watts = Nm/s Is the following correct? Since Watts = Volts*Amps And Nm/s could be written as Force * speed: Volts = Speed Amps = Force The notion about Amps representing force (converted to torque in a motor) and Volts representing speed is new to me, and I've had some difficulties wrapping my head around it. Amps is ok, I know lots of Amps give high torque, but how could volts represent speed? I mean as you can derive from Newtons first law, if no energy is added or subracted, the speed should remain constant. And this is probably where I'm wrong, but this says to me that Volts (speed) is irrelevant as long as you have the amps to do the work. I'm afraid there is no real world purpose for my inquiry, but rather a need to clean up a messy corner of my mind :-) There is however several examples where I could try to put this new info to good use. Going back to the propeller (Helicopter, plane or other) I can accept that the prop will need Amps (Torque) to push it around against the air, and Volts to keep the prop speed up. Am I getting closer to home, or still hopelessly lost? |
| Mar5-10, 10:18 PM | #43 |
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Here is one flaw in your reasoning. Multiplication is commutative, meaning that the order in which two things are multiplied doesn't matter. So, although you have written that power = voltage*current, you could just have easily have written that power = current*voltage, which would have led you to conclude something entirely different using your "matching" procedure. But, more fundamentally, just because two pairs of multiplied quantities both happen to have dimensions of power doesn't mean that those two pairs of quantities are the same! I didn't slog through this whole thread, but just to be sure, you do realize that it possible for a motor to use up (i.e. to waste) electrical energy without doing any useful work, right? |
| Mar5-10, 11:44 PM | #44 |
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electrical potential energy between two points is the negative of the work done by an electrical field from point0 to point1. electrical intensity is the electrical force per unit charge of some target object, considering the source object as the generator of an electrical field. voltage = the difference between electrical potential energy per unit charge between two points, one of which can be a "reference" point. current = the rate of charge flow across some point or between two points. power = force x speed doesn't directly translate well into power = volts x current. Analogy using an infinitely large disk with a finite negative charge or finite amount of gravity per unit area, and "h" as distance from that disk: Intensity= -E (newtons / coulomb) => gravitational intensity = -g (newtons / kilogram) Force = -Eq => -gm volt = joule / coulomb potential = V (volts) = Eh => gh = V (joule / kilogram) potential energy = U (joules) = Eqh => gmh = U (joules) Power for a moving fixed amount of charge or mass: power = |-Eq (dh/dt)| = |-q (dV/dt)| => |-gm (dh/dt)| = |-m (dV/dt)| Power for a constant flow of charge or mass bewteen two points in space: I = dq/dt ṁ = dm/dt power = E (dq/dt) (dh/dt) = (dq/dt) (dV/dt) = I (dV/dt) => g (dm/dt) (dh/dt) = (dm/dt) (dV/dt) = ṁ (dV/dt) let V = dV/dt = amount of change in potential per unit time. power = I V = current x voltage_change => ṁ V = mass_flow x gravitaional_potential_change let q = dq/dt = amount of charge that flows betwen two points per unit time. let m = dq/tm = amount of mass that flows between two points per unit time. power = Eq (dh/dt) => gm (dh/dt) => force x speed. |
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