  Using the effective Lagrangian approach, we examine the recently observed
charm states $D^{*}_{J}(2460)$, $D_{J}(2560)$, $D_{J}(2740)$, $D_{J}(3000)$ and
their spin partners $D^{*}_{J}(2680)$, $D^{*}_{J}(2760)$ and $D^{*}_{J}(3000)$
with $J^{P}$ states $1P_{\frac{3}{2}}2^{+}$, $2S_{\frac{1}{2}}0^{-}$,
$1D_{\frac{5}{2}}2^{-}$, $2P_{\frac{1}{2}}1^{+}$ and $2S_{\frac{1}{2}}1^{-}$,
$1D_{\frac{5}{2}}3^{-}$, $2P_{\frac{1}{2}}0^{+}$ respectively. We study their
two body strong decays, coupling constants and branching ratios with the
emission of light pseudo-scalar mesons $(\pi, \eta, K)$. We also analyze the
newly observed charm state $D^{*}_{2}(3000)$ and suggest it to be either
$1F(2^{+})$ or $2P(2^{+})$ state and justify one of them to be the most
favorable assignment for $D^{*}_{2}(3000)$. We study the partial and the total
decay width of unobserved states $D(1^{1}F_{3})$, $D_{s}(1 ^{1}F_{3})$ and
$D_{s}(1 ^{1}F_{2})$ as the spin and the strange partners of the
$D^{*}_{2}(3000)$ charmed meson. The branching ratios and the coupling
constants $g_{TH}$, $\widetilde{g}_{HH}$, $g_{YH}$, $\widetilde{g}_{SH}$ and
$g_{ZH}$ calculated in this work can be confronted with the future experimental
data.
