Power equation in railgun operation

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Discussion Overview

The discussion revolves around the power equation in the operation of railguns, particularly focusing on the relationship between the power supplied by a capacitor bank and the kinetic energy transferred to the armature. Participants explore the complexities of modeling railgun operation, including the roles of inductance and ohmic losses.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • Some participants note that the power supplied by the capacitor (VI) must account for ohmic losses (I²R) in the rails and armature, raising questions about how kinetic energy is also included in the power equation.
  • Others argue that inductance plays a significant role in electro-mechanical systems like railguns, suggesting that additional losses and energy transfer mechanisms must be considered beyond simple circuit analysis.
  • A participant expresses interest in understanding how power from the capacitor bank is converted to kinetic energy and what factors contribute to ohmic losses.
  • Some participants reference existing literature and resources, suggesting that a foundational understanding of electromagnetism and circuit analysis is necessary to grasp the complexities of railgun operation.
  • One participant compares railguns to DC motors, suggesting that understanding the operation of motors may help in understanding railguns, although they acknowledge the differences in application.
  • A later reply discusses the role of magnetic flux and back emf in the context of railgun operation, mentioning Lenz's law and the Lorentz force as relevant concepts, although there is some confusion about terminology.

Areas of Agreement / Disagreement

Participants express varying levels of understanding and readiness to engage with the complexities of railgun operation. There is no consensus on a simplified explanation or a unified model, and multiple viewpoints regarding the role of inductance and energy transfer remain present.

Contextual Notes

Some participants indicate that a solid grasp of basic electromagnetism, differential equations, and LCR circuit analysis is essential for deeper discussions, suggesting that the conversation may be limited by differing levels of background knowledge among participants.

avicenna
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In a capacitor discharge through a plain resistor, the capacitor power supplied at any instant is VI; the power dissipated in the resistor is I²R. So VI = I²R.

Consider a railgun operated with a capacitor bank. At any instant of capacitor discharge, the power supplied is VI. The total power supplied for ohmic loss is sum I²R for two rails plus the resistance of the armature.

Question: Since VI = total I²R, how can the power equation include the kinetic energy supplied to the armature?
 
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avicenna said:
In a capacitor discharge through a plain resistor, the capacitor power supplied at any instant is VI; the power dissipated in the resistor is I²R. So VI = I²R.

Consider a railgun operated with a capacitor bank. At any instant of capacitor discharge, the power supplied is VI. The total power supplied for ohmic loss is sum I²R for two rails plus the resistance of the armature.

Question: Since VI = total I²R, how can the power equation include the kinetic energy supplied to the armature?
The short answer is that in electro-mechanical machines, like motors or railguns, there is a significant inductance term in the equations and additional losses associated with the energy transferred. Your schematic may look like an RC discharge, but there are other effects that need to be included in your model.

Beware of using circuit analysis before you've worked out the fundamental physics in the system. The circuits are just a simplified, standardized, representation of the real world. They are just a way of telling other EEs "you don't have to worry about physics, I've already done that for you."*

Personally, I'm a big fan of google searches. Here's (literally) the first result for "railgun electrical model". Look at figure 2.

* This concept, BTW, is something many physicist don't understand. But I'll spare y'all my diatribe on that.
 
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DaveE said:
The short answer is that in electro-mechanical machines, like motors or railguns, there is a significant inductance term in the equations and additional losses associated with the energy transferred. Your schematic may look like an RC discharge, but there are other effects that need to be included in your model.

Beware of using circuit analysis before you've worked out the fundamental physics in the system. The circuits are just a simplified, standardized, representation of the real world. They are just a way of telling other EEs "you don't have to worry about physics, I've already done that for you."*

Personally, I'm a big fan of google searches. Here's (literally) the first result for "railgun electrical model". Look at figure 2.

* This concept, BTW, is something many physicist don't understand. But I'll spare y'all my diatribe on that.
The link you gave involves a mathematical modeling with mathematics beyond me.

I would be interested if anyone could provide a simplified explanation as to how some of the power of the capacitor bank is transferred to kinetic energy in the armature. And what factors determined how much power are wasted as ohmic loss.
 
DaveE said:
Still, I don't know that we can do better than what's already out there.
https://en.wikipedia.org/wiki/Railgun
https://science.howstuffworks.com/rail-gun1.htm

If you haven't studied basic EM (like Faraday's law, etc.), basic differential equations, and LCR circuit analysis, I think you might not really be ready for the "how does it work question".
I could understand how motors, generators, transformer, capacitor, faraday's law, etc. work.

As for railguns, since there cannot be a simplified "layman" answer, I don't think I am ready to ask the question.
 
I don't think it's too different than a DC motor. If you really understand motors that spin, I'm sure you can figure out linear motors and railguns. The basic concepts are mostly the same.
 
The key point with railguns is that when the current starts to flow it creates an increase in the magnetic flux. But "nature resists a change in magnetic flux", so that creates either (or both) a back emf (voltage) to oppose the current increase (this is inductance) and a force on the conductors to increase the area enclosed by the current. This is because flux is inversely proportional to area; if the current increases by 10% but the area also increases by 10%, then the flux doesn't change. Since one of the conductor in the rail gun loop is the arc between the rails, then this makes a force to push the arc away along with whatever projectile is in the way. I think it's Lenz's law, but I get confused about the names of these things.

Edit: not Lenz, Lorentz force is a better name.
 
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