Can someone explain the 4-force to me.

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Discussion Overview

The discussion centers around the concept of the 4-force in the context of relativity, exploring its definition, components, and practical implications. Participants express confusion regarding the utility of the 4-force compared to traditional force concepts, as well as the significance of its time component.

Discussion Character

  • Exploratory, Technical explanation, Debate/contested

Main Points Raised

  • Some participants express uncertainty about the benefits of using the 4-force and question its practical applications.
  • One participant highlights the relationship between the change in momentum and the 4-force, suggesting that it is useful.
  • Another participant discusses the energy-momentum four-vector and its components, noting confusion about the physical significance of the fourth piece of the vector.
  • There is mention of the tediousness of converting between ordinary force and four-force, with a preference expressed for using either four-vectors or three-vectors exclusively.
  • One participant seeks clarification on the time component of the four-force, relating it to the power exerted by the force.
  • A participant reflects on a relativistic energy conservation problem, indicating they may have only needed the 3-vector for their solution.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the utility and significance of the 4-force, with multiple competing views and ongoing confusion about its components and applications.

Contextual Notes

Participants express limitations in their understanding of the definitions and implications of the 4-force and its components, particularly the time piece, without resolving these uncertainties.

ozone
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I understand that we can write the 4-force in terms of the vector force based on velocity, and the energy of the system in general.

What I don't understand is what this gains for us, and why we use it. Also correct me if I am incorrect in my definition above.. I don't have my book infront of me.
 
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Knowing [itex]dp/d\tau = f[/itex] isn't useful?
 
no that's very useful. I don't understand though why we have a vector we call the energy-momentum four-vector,

defined as
[itex]p = (E, p)[/itex]

Where the vector p is just our ordinary momentum.

Also we have a 4-vector force defined as
[itex]f = (\gamma F \cdot V, \gamma \text{ }F)[/itex]

Obviously both terms contain standard 3-vector, but I'm not sure what physical good the fourth piece is.

This is out of James Hartle's Intro to relativity.
 
I'm not sure I understand what "fourth" piece you're referring to.

At any rate, I find the formulas for converting between ordinary force and four-force (and the same for acceleration) to be very annoying and tedious. I personally try to avoid dealing in ordinary force and acceleration precisely for this reason. It's just much easier to deal only with four-vectors or only with three-vectors and not constantly convert back and forth between them.
 
The fourth piece (the time piece) is just confusing to me.. I understand having momentum in terms of velocity but my book doesn't really explain why/what the 4th piece of the vector is.

Also I solved a relativistic energy conservation problem (in the lab frame) and I am pretty sure I only needed to use the 3-vector but I want to make sure that I did that correctly.
 
The time component of the four-force is basically the power the force applies to the object in question.
 

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