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This is a page from Sean Carroll's Spacetime and Geometry.There is a line in this page which says that the four velocity is automatically normalized.This absolute normalization is a reflection of the fact that the four-velocity is not velocity through space,which can of course take on different magnitude,but a velocity through spacetime through which one travels at the same speed.

  1. What is the absolute normalization here?

  2. How four-velocity is automatically normalized?

  3. Is four velocity always a unity?

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  • $\begingroup$ He's using natural units here, normally that $1$ would be a $c^2$ $\endgroup$ – Craig Jan 17 at 15:08
  • $\begingroup$ Possible duplicates: physics.stackexchange.com/q/410603/2451 and links therein. $\endgroup$ – Qmechanic Jan 17 at 15:12
  • $\begingroup$ Please don't post questions using images of text. It breaks search functionality and adaptive technology for the blind. $\endgroup$ – Ben Crowell Jan 17 at 15:57
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Written out, the four-velocity's four components are $\frac{dt}{d\tau}$ and the 3-vector $\frac{d\vec{x}}{d\tau}$. Note that $\frac{dt}{d\tau}=\gamma$, and $\frac{dx_i}{d\tau}=\frac{dx_i}{dt}\frac{dt}{d\tau}=\beta_i\gamma$, where we set $c=1$ as usual.

When we take the "length" of this vector under the Minkowski metric $\eta_{\mu\nu}$, we get (using the signature $(-,+,+,+)$ as Carroll uses here):

\begin{align} \eta_{\mu\nu}U^\mu U^\nu&= -\left(\frac{dt}{d\tau}\right)^2+\left(\frac{d\vec{x}}{d\tau}\right)^2\\ &=-\gamma^2+(\beta_x^2+\beta_y^2+\beta_z^2)\gamma^2\\ &=-\gamma^2(1-\beta^2)\\ &=-1 \end{align}

where the last line is derived from the fact that $\gamma=\frac{1}{\sqrt{1-\beta^2}}$. So the "length" of this 4-vector under the Minkowski metric is always $-1$ under these conventions. (If you were to use the other convention for defining the metric, with signature $(+,-,-,-)$, then the "length" of this 4-vector would be $1$).

It is "automatically" normalized because its normalization comes directly from its definition. The relationship between proper time and time in other frames guarantees that when you change frames, any change in the four-velocity's length from time dilation is exactly cancelled by an equal and opposite change in the four-velocity's length due to length contraction.

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