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We study the semi-leptonic and non-leptonic decays of $B_c$ meson to $D$-wavecharmonia, namely, $\eta_{c2}(1^1\!D_2)$, $\psi_2(1^3\!D_2)$, and$\psi_3(1^3\!D_3)$. In our calculations, the instantaneous Bethe-Salpetermethod is applied to achieve the hadronic matrix elements. This method includesrelativistic corrections which are important especially for the higher orbitalexcited states. For the semi-leptonic decay channels with electron as the finallepton, we get the branching ratios $\mathcal{B}[B_c \rightarrow\eta_{c2}e\bar{\nu}_e] = 5.9^{-0.8}_{+1.0}\times 10^{-4}$, $\mathcal{B}[B_c\rightarrow \psi_2e\bar{\nu}_e]=1.5^{-0.2}_{+0.3}\times 10^{-4}$, and$\mathcal{B}[B_c \rightarrow \psi_3e\bar{\nu}_e]=3.5^{-0.6}_{+0.8}\times10^{-4}$. The transition form factors, forward-backward asymmetries, and leptonspectra in these processes are also presented. For the non-leptonic decaychannels, those with $\rho$ as the lighter meson have the largest branchingratios, $\mathcal{B}[B_c \rightarrow \eta_{c2}\rho] = 8.1^{-1.0}_{+1.0}\times10^{-4}$, $\mathcal{B}[B_c \rightarrow \psi_2\rho]=9.6^{-1.0}_{+1.0}\times10^{-5}$, and $\mathcal{B}[B_c \rightarrow \psi_3\rho]=4.1^{-0.7}_{+0.8}\times10^{-4}$.

$D$-Wave Charmonia $\eta_{c2}$($1{^1D_2}$), $\psi_2$($1{^3D_2}$), and $\psi_3$($1{^3D_3}$) in $B_c$ Decays