(d) The electric displacement field is a vector valued D that accounts for the effects of bound charges within materials. In general D is given by
$\mathbf{D} = \varepsilon_{0}\mathbf{E\ } + \mathbf{\ P}$
When E is electric field,$\varepsilon_{0}$ the vacuum permittivity and P the polarization density of the material.
In most ordinary terms
$\mathbf{D} = \varepsilon_{0}\mathbf{E}$
When dielectric is present $\varepsilon = K\varepsilon_{0}$
$\mathbf{\therefore\ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ D} = K\varepsilon_{0}\mathbf{E}$