  The gauge couplings $WWZ$, $WWWW$, and $WWZZ$ in the gauge-Higgs unification
scenario in the Randall-Sundrum warped spacetime remain almost universal as in
the standard model, but substantial deviation results for the Higgs couplings.
In the $SO(5)\times U(1)_{B-L}$ model, the couplings $WWH$ and $ZZH$ are
suppressed by a factor $\cos \theta_H$ from the values in the standard model,
while the bare couplings $WWHH$ and $ZZHH$ are suppressed by a factor
$1-(2/3)\sin^2 \theta_H$. Here $\theta_H$ is the Yang-Mills AB phase (Wilson
line phase) along the fifth dimension, which characterizes the electroweak
symmetry breaking. The suppression can be used to test the gauge-Higgs
unification scenario at LHC and ILC. It is also shown that the $WWZ$ coupling
in flat spacetime deviates from the standard model value at moderate values of
$\theta_H$, contradicting with the LEP2 data.
