SR: magnitude of a particle's 3-momentum

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Homework Help Overview

The problem involves the calculation of the magnitude of a particle's 3-momentum as observed by an experimentalist, utilizing concepts from special relativity, specifically 4-velocity and 4-momentum. The original poster presents a mathematical expression and seeks clarification on a potential discrepancy in the formulation found in a textbook.

Discussion Character

  • Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • The original poster attempts to derive the expression for the magnitude of the 3-momentum and questions the validity of the textbook's formulation, particularly regarding the power of the term involving the scalar product of the 4-momentum.

Discussion Status

Participants are engaged in examining the original poster's derivation and the potential error in the textbook. Some express skepticism about the correctness of the textbook's equation, suggesting it may contain a typo. There is an ongoing exploration of the implications of the dimensional consistency of the terms involved.

Contextual Notes

Participants note the use of units where the speed of light, c, is set to 1, which is relevant to the equations being discussed. The discussion also highlights the importance of ensuring dimensional consistency in the expressions used.

lomidrevo
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Homework Statement


We observe an experimentalist moving by with 4-velocity ##u^\mu## and a particle zipping by with 4-momentum ##p^\mu##. Show that magnitude of the particle's 3-momentum as seen by the experimentalist is given by
$$ |\vec p| = \left [ (p \cdot u)^2 + (p \cdot p)^2 \right ] ^{1/2}$$

Homework Equations


Scalar dot product between 4-vectors:
##p \cdot q = -p^0q^0 + p^1q^1 + p^2q^2 + p^3q^3 = -p^0q^0 + \vec p \cdot \vec q##

The Attempt at a Solution


Let's denote our reference frame as unprimed, and the experimentalist's frame of reference as primed. As the scalar dot product between two 4-vectors is invariant under Lorentz's transformation we can write:
##p \cdot p = p' \cdot p' = -p'^0p'^0 + \vec p' \cdot \vec p'##
##p \cdot u = p' \cdot u' = -p'^0u'^0 + \vec p' \cdot \vec u'##
but in the experimentalist frame of reference ##u'^\mu = (1, \vec 0)##, therefore the second equation can be written as:
##p \cdot u = p' \cdot u' = -p'^0##
and combining with the first equation, we get:
##\vec p' \cdot \vec p' = (p \cdot u)^2 + (p \cdot p)##
expressing for the magnitude of the 3-momentum as seen in the experimentalist's reference frame:
##|\vec p'| = \sqrt{(p \cdot u)^2 + (p \cdot p)}##

In the problem statement the ##(p \cdot p)^2## comes with power of 2 under the square root, in my solution it comes only with power of 1: ##(p \cdot p)##. Could you pls have a look at my solution and to advice whether I am wrong at some point? Or possibly, is there a typo in the textbook from where I got this problem?

Note: I believe it is obvious, but better to emphasize it: author uses such units, that ##c=1## and therefore it is omitted in the equations.
 
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The square in the ##p\cdot p## term leads to a dimensional inconsistency and is therefore quite clearly wrong.
 
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lomidrevo said:
Or possibly, is there a typo in the textbook from where I got this problem?

As pointed out above, the book solution is wrong. I suspect the author got caught between writing ##p.p## and ##p^2##.
 
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@Orodruin, @PeroK, thank you! I've suspected that the equation in the textbook might be wrong, but wasn't sure about that.
 

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