  The first results on K$^{*}$(892)$^{\mathrm{\pm}}$ resonance production in
inelastic pp collisions at LHC energies of $\sqrt{s} = 5.02$, 8, and 13 TeV are
presented. The K$^{*}$(892)$^{\mathrm{\pm}}$ has been reconstructed via its
hadronic decay channel K$^{*}$(892)$^{\mathrm{\pm}}$ $\rightarrow$ $\mathrm
{K^0_S}$ $~+~\pi^{\pm}$ with the ALICE detector. Measurements of transverse
momentum distributions, $p_{\mathrm{T}}$-integrated yields, and mean transverse
momenta for charged K$^{*}$(892) are found to be consistent with previous ALICE
measurements for neutral K$^{*}$(892) within uncertainties. For $p_{\mathrm{T}}
> 1$ GeV/$c$ the K$^{*}$(892)$^{\mathrm{\pm}}$ transverse momentum spectra
become harder with increasing centre-of-mass energy from 5.02 to 13 TeV,
similar to what previously observed for charged kaons and pions. For
$p_{\mathrm{T}} < 1$ GeV/$c$ the K$^{*}$(892)$^{\mathrm{\pm}}$ yield does not
evolve significantly and the abundance of K$^{*}$(892)$^{\mathrm{\pm}}$
relative to K is rather independent of the collision energy. The transverse
momentum spectra, measured for K$^{*}$(892)$^{\mathrm{\pm}}$ at midrapidity in
the interval $0 < p_{\mathrm{T}} < 15$ GeV/$c$, are not well described by
predictions of different versions of PYTHIA 6, PYTHIA 8 and EPOS-LHC event
generators. These generators reproduce the measured $p_{\mathrm{T}}$-integrated
K$^{*\mathrm{\pm}}$/K ratios and describe well the momentum dependence for
$p_{\mathrm{T}} < 2$ GeV/$c$.
