Covariant vs. contravariant time component

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The discussion focuses on the identification of the energy of a particle with the time component of the four-momentum vector, specifically p^0 versus p_0. It highlights that while p^0 and p_0 are equal in the standard metric (+---), they differ in other metrics like the Schwarzschild metric, affecting their magnitudes and implications for energy representation. The conversation also touches on the use of covariant versus contravariant forms in different metrics and the significance of ensuring positive energy values. Additionally, it raises questions about the interpretation of the timelike Killing vector and its relation to the energy expression along a particle's worldline. The complexity of these relationships underscores the importance of metric choice in relativistic physics.
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...of the four-momentum vector.

Why is the energy of a particle identified with p0 instead of p0? Is there a theoretical basis for this, or was it simply observed that p0 is conserved in a larger set of circumstances?
 
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How is the metric written in that book (-+++) or (+---)?

Covariant and contravariant components are related by the metric.

Just make sure the energy is positive.
 
In the more usual metric (+---) of SR, p^0 and p_0 are equal, so it doesn't matter which you use. In any event, although they are equal, it should be p^0 that is the physical energy since the four-momentum is a contravariant vector.
If you are reading a book that uses the metric (-+++), then everything could be different.
 
I did not have the Minkowski metric specifically in mind. If one uses the Schwarzschild metric -- or any other diagonal metric with |g_{00}|\neq1 -- p0 and p0 differ by more than just the sign; they have different magnitudes, so the energy of a particle cannot have both values. It's been my impression that in such circumstances one uses the covariant form instead of the contravariant form, but I don't know why.
 
snoopies622 said:
If one uses the Schwarzschild metric

If one uses standard Schwarzschild coordinates, then

k = \frac{\partial}{\partial t}

is a timelike Killing vector. If u is the 4-velocity of a freely falling particle, then

E = g \left( k , u \right)

is constant along the particle's worldline.

What is the coordinate expression of the above coordinate-free expression?
 
What I had in mind was

p^0=m_0 c \frac{dt}{d\tau} while p_0= g_{00}m_0 c \frac{dt}{d\tau}=(1-\frac{r_s}{r})m_0 c \frac{dt}{d\tau}

where d\tau=ds/c and ds is defined using the Schwarzschild metric. Since (1-\frac{r_s}{r}) won't equal 1 while r is finite, these two terms (p0 and p0) have different values, and I don't know which one (if either) represents the energy of the particle.

Regarding the coordinate-free expression, when you say that k = \frac{\partial}{\partial t} is a vector, do you mean the partial derivative of the displacement vector with respect to coordinate time? or of a different vector?
 
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