An analysis with a transferred hyperfine field has been performed on the spectra of the $^{115}\mathrm{In}$ nuclear quadrupole resonance experiments of heavy fermion superconductor ${\mathrm{Ce}}_{3}{\mathrm{PtIn}}_{11}$ exhibiting co-occurrence of two successive antiferromagnetic orderings (${T}_{\mathrm{N}1}$ = 2.2 K and ${T}_{\mathrm{N}2}$ = 2.0 K) followed by a superconducting transition (${T}_{\mathrm{c}}$ = 0.32 K). The spectral changes at magnetic transition temperatures ${T}_{\mathrm{N}1}$ and ${T}_{\mathrm{N}2}$ indicate that the Ce(2) site has the dominant magnetic contribution, with a small magnetic moment, but not negligible, at the Ce(1) site. Our analysis using a transferred hyperfine field which overcomes the previous simple dipolar model evinces the magnetic structures of ${\mathrm{Ce}}_{3}{\mathrm{PtIn}}_{11}$. $\mathrm{For}{T}_{\mathrm{N}2}<T<{T}_{\mathrm{N}1}$, the propagation vectors at the Ce(1) and Ce(2) sublattices are ${\mathbit{q}}_{1}={\mathbit{q}}_{2}=(\frac{1}{2},\phantom{\rule{0.16em}{0ex}}\frac{1}{2},\phantom{\rule{0.16em}{0ex}}0\phantom{\rule{0.16em}{0ex}}\phantom{\rule{4.pt}{0ex}}\text{or}\phantom{\rule{4.pt}{0ex}}\phantom{\rule{0.16em}{0ex}}\frac{1}{2})$. On the other hand, for $T<{T}_{\mathrm{N}2}$, the propagation vectors are ${\mathbit{q}}_{1}=(\frac{1}{2},\phantom{\rule{0.16em}{0ex}}\frac{1}{2},\phantom{\rule{0.16em}{0ex}}\frac{1}{6}\phantom{\rule{0.16em}{0ex}}\text{or}\phantom{\rule{4.pt}{0ex}}\phantom{\rule{0.16em}{0ex}}\frac{1}{3})$ and ${\mathbit{q}}_{2}=(\frac{1}{2},\phantom{\rule{0.16em}{0ex}}\frac{1}{2},\phantom{\rule{0.16em}{0ex}}\frac{1}{2}\phantom{\rule{0.16em}{0ex}}\phantom{\rule{4.pt}{0ex}}\text{or}\phantom{\rule{4.pt}{0ex}}\phantom{\rule{0.16em}{0ex}}0)$, respectively.