  In d$_{x^2-y^2}$-wave superconductors, the effect of s-wave point disorder
has been extensively studied in the literature. In this work, we study the
anisotropic disorder with a the form of $V_{kk'}^{\rm imp}=V_if_kf_{k'}$ with
$f_k=\cos(2\theta)$ (with $\theta$ the azimuthal angle of $k$), as proposed to
be caused by apical oxygen vacancies in overdoped La-based cuprate films, under
the Born approximation. The disorder self-energy and d-wave pairing affect each
other and have to be solved simultaneously self-consistently. We find the
self-energy is reduced at low frequencies and thus weakens the pair-breaking
effect. This frequency-dependence vanishes in the dirty limit for which the
disorder is well described by a scattering rate $\Gamma_k=\Gamma_if_k^2$. One
consequence of the disorder effect is the gap-to-$T_c$ ratio $2\Delta(0)/T_c$
is greatly enhanced by the d-wave disorder, much larger than the s-wave
disorder and the clean BCS value $4.28$. At last, we generalize the d-wave
scattering rate to a general form
$\Gamma_\theta=\Gamma_\alpha|\theta-\theta_0|^\alpha$ around each nodal
direction $\theta_0$. We find the density of states
$\rho(\omega)-\rho(0)\propto|\omega|$ ($\omega^2$) for all $\alpha\ge1$
($\alpha<1$) in the limit of $\omega\to0$. As a result, the superfluid density
$\rho_s$ exhibits two and only two possible scaling behaviors:
$\rho_s(0)-\rho_s(T)\propto T$ ($T^2$) for $\alpha\ge1$ ($\alpha<1$) in the low
temperature limit.
