  The form factors of $\gamma^* N \rightarrow \Delta(1600)$ transition is
calculated within the light-cone sum rules assuming that $\Delta^+(1600)$ is
the first radial excitation of $\Delta(1232)$. The $Q^2$ dependence of the
magnetic dipole $\tilde{G}_M(Q^2)$, electric quadrupole $\tilde{G}_E(Q^2)$, and
Coulomb quadrupole $\tilde{G}_c(Q^2)$ form factors are investigated. Moreover,
the $Q^2$ dependence of the ratios $R_{EM} =
-\frac{\tilde{G}_E(Q^2)}{\tilde{G}_M{Q^2}}$ and $R_{SM} = - \frac{1}{4
m_{\Delta(1600)}^2} \sqrt{4 m_{\Delta(1600)}^2 Q^2 + (m_{\Delta(1600)}^2 - Q^2
- m_N^2)^2} \frac{\tilde{G}_c(Q^2)}{\tilde{G}_M(Q^2)}$ are studied. Finally,
our predictions on $\tilde{G}_M(Q^2)$, $\tilde{G}_E(Q^2)$, and
$\tilde{G}_C(Q^2)$ are compared with the results of other theoretical
approaches.
