$\newcommand{\bbx}[1]{\,\bbox[15px,border:1px groove navy]{\displaystyle{#1}}\,}
\newcommand{\braces}[1]{\left\lbrace\,{#1}\,\right\rbrace}
\newcommand{\bracks}[1]{\left\lbrack\,{#1}\,\right\rbrack}
\newcommand{\dd}{\mathrm{d}}
\newcommand{\ds}[1]{\displaystyle{#1}}
\newcommand{\expo}[1]{\,\mathrm{e}^{#1}\,}
\newcommand{\ic}{\mathrm{i}}
\newcommand{\mc}[1]{\mathcal{#1}}
\newcommand{\mrm}[1]{\mathrm{#1}}
\newcommand{\pars}[1]{\left(\,{#1}\,\right)}
\newcommand{\partiald}[3][]{\frac{\partial^{#1} #2}{\partial #3^{#1}}}
\newcommand{\root}[2][]{\,\sqrt[#1]{\,{#2}\,}\,}
\newcommand{\totald}[3][]{\frac{\mathrm{d}^{#1} #2}{\mathrm{d} #3^{#1}}}
\newcommand{\verts}[1]{\left\vert\,{#1}\,\right\vert}$
With $\ds{U_{1} = DE}$:
\begin{align}
U_{n} & = \pars{U_{n - 1} + D}E \implies
U_{n} - {DE \over 1 - E} = \pars{U_{n - 1} - {DE \over 1 - E}}E =
\pars{U_{n - 2} - {DE \over 1 - E}}E^{2}
\\[5mm] & =
\pars{U_{n - 3} - {DE \over 1 - E}}E^{3} = \cdots =
\pars{U_{1} - {DE \over 1 - E}}E^{n - 1} =
\pars{DE - {DE \over 1 - E}}E^{n - 1}
\\[5mm] & = {D \over E - 1}\,E^{n + 1} \implies
U_{n} = {DE \over 1 - E} + {D \over E - 1}\,E^{n + 1} =
\bbx{DE\,{E^{n} - 1 \over E - 1}}
\end{align}