Minimum energy to accelerate a mass?

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SUMMARY

The discussion centers on the minimum energy required to accelerate a mass, particularly in the context of Special Relativity (SR). It is established that the energy of a massive particle moving at velocity v is given by the equation E=γmc², where γ=(1-v²/c²)⁻¹/². The conversation highlights that the energy increases as the mass approaches the speed of light (c), with the first term representing rest mass energy and subsequent terms representing kinetic energy and relativistic effects. The measurable effects of this energy increase become significant as velocity approaches a substantial fraction of c.

PREREQUISITES
  • Understanding of Special Relativity (SR)
  • Familiarity with the equation E=γmc²
  • Knowledge of Taylor series expansions
  • Basic concepts of kinetic energy and relativistic effects
NEXT STEPS
  • Study the implications of the Lorentz factor (γ) in relativistic physics
  • Explore the concept of relativistic kinetic energy and its derivation
  • Investigate the precision of modern energy measurement devices in high-velocity contexts
  • Examine Minkowski diagrams for visualizing relativistic effects
USEFUL FOR

Physics students, educators, and anyone interested in the principles of Special Relativity and the energy dynamics of accelerating masses.

jerromyjon
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I have a similar logical "gap" in my understanding that I still haven't resolved... which seems to be right on point with this thread if I call it "minimum amount of energy required to accelerate a given mass".

From what I know about SR, accelerating mass takes energy which increases exponentially as this mass approaches c. I just don't know at what speed this effect becomes measurable...
 
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jerromyjon said:
I have a similar logical "gap" in my understanding that I still haven't resolved... which seems to be right on point with this thread if I call it "minimum amount of energy required to accelerate a given mass".

From what I know about SR, accelerating mass takes energy which increases exponentially as this mass approaches c. I just don't know at what speed this effect becomes measurable...
It isn't an exponential growth. The energy of a massive particle moving at velocity v is E=\gamma mc^2, where \gamma=(1-v^2/c^2)^{-1/2}. If you Taylor expand the expression for \gamma you get
E=mc^2<br /> +\frac{1}{2}mv^2<br /> +\frac{3}{4}m<br /> \frac{v^4}{c^2}<br /> +...The first term is mass energy. The second is Newtonian kinetic energy. The third and later terms are where relativity disagrees with Newton on energy. So the effect is measurable when that term is measurable.

I don't know if there's an answer to your question in practical terms since I'm not current on the precision of energy measurement devices, and that probably depends on your application anyway. But that's the theoretical basis for an answer.
 
Thank you, I appreciate your response! I'm still trying to learn what is still "greek" to me, but that funky y that you all call gamma... isn't that only zero at zero velocity?
 
jerromyjon said:
gamma... isn't that only zero at zero velocity?

What do you get when you plug v = 0 into the formula for gamma? $$\gamma = \frac{1}{\sqrt{1 - v^2/c^2}}$$
 
Ummm, If I set c=1 then its 1 but I'm not even sure about that c=1 scenario.
 
oh duh nevermind gamma has to be 1 to be at rest energy..
 
Ok. So what I meant was gamma is 1 at rest energy, which would only be at rest velocity. Suppose we do the M&M set-up with "identical" rockets in opposite directions, along with an identical complete system at a known relative velocity parallel to the launch vectors. This is where I'm unsure how to predict how this system evolves, but now I recall something about the relativistic "tether" problem, where the distance changes, severely complicating this visually. I'm going to play with that interactive Minkowski diagram (Thanks Ibix!) and see if I can figure it out...
 

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