The reciprocal bootstrap relationship of the octet of ${(\mathrm{\textonehalf{}})}^{+}$ baryons and the decuplet of ${(\frac{3}{2})}^{+}$ baryons is studied making use of the static approximation. If we regard the octet baryon as a ${B}_{8}{\ensuremath{\Pi}}_{8}$ bound state due to octet and decuplet baryon exchange, we obtain ${\ensuremath{\gamma}}_{10}\ensuremath{\approx}7{d}^{2}$ and $\frac{d}{f}\ensuremath{\approx}2.2$, where ${\ensuremath{\gamma}}_{10}$ is the ${\overline{B}}_{10}{B}_{8}{\ensuremath{\Pi}}_{8}$ coupling constant and $d$ and $f$ are the $d$ and $f$ coupling constants of ${\overline{B}}_{8}{B}_{8}{\ensuremath{\Pi}}_{8}$ coupling. If octet vector meson exchange processes are included and if we assume the vector theory (gauge theory) of strong interactions, we obtain ${\ensuremath{\gamma}}_{10}l7{d}^{2}$ and $\frac{d}{f}l2.2$. If we regard the decuplet baryon as a ${B}_{8}{\ensuremath{\Pi}}_{8}$ bound state due to octet baryon exchange, we obtain ${\ensuremath{\gamma}}_{10}\ensuremath{\approx}4{d}^{2}$ for the ratio $\frac{d}{f}=2.2$.