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A classical particle is always on-shell and thus you have
$$g_{\mu \nu} u^{\mu} u^{\nu}=1$$
since
$$u^{\mu}=\frac{1}{m} p^{\mu},$$
where ##p^{\mu}## is the momentum of the particle.
The four-velocity is always time like and ##u^0 >0## by convention, i.e., you take the proper time defining the same causal time direction as the coordinate time.
$$g_{\mu \nu} u^{\mu} u^{\nu}=1$$
since
$$u^{\mu}=\frac{1}{m} p^{\mu},$$
where ##p^{\mu}## is the momentum of the particle.
The four-velocity is always time like and ##u^0 >0## by convention, i.e., you take the proper time defining the same causal time direction as the coordinate time.