The idea is that tidal deformation (gravitational gradients) can increase strain, thereby triggering strain-relief: a quake.
In the extreme case of the Earth passing inside the Roche limit of a larger ($M$) celestial body, the answer is clearly "yes".
For instance, a rogue black hole would produce a gradient large enough to induce The Rapture (people on the line of syzygy would be lifted off the surface on both sides of the planet, those transverse to that would be pulled down into the crumbling crust, for a red hot molten demise...have I read the somewhere before?).
In more mundane circumstances, tidal gradients go as:
$$ \frac{ M }{R^3} $$
The sun competes with $M$, while the moon wins "out" on $R$. From there, look at the planets and see their relative contribution.
Being a tensor alignment, direction doesn't matter, so if Venus and Jupiter line up: they add, even though they are on opposite sides of the planet.
You just have to plug in the numbers.
Edit (based on comments):
With a gravitational potential $U(\vec x)$, the Hessian is:
$$ J_{ij} = \frac{\partial^2 U}{\partial x_i \partial x_j} $$
The tidal tensor is the symmetric trace free (aka "natural rank-2 tensor"):
$$ \Phi_{ij} = J_{ij} - \frac 1 3 {\rm Tr}(J) $$
which has 5 components. These induce quadruple deformations in the Earth's shape that are characterized by the 5 (real) spherical harmonics with $l=2$... e.g. prolate stretching. Because it's traceless, the longitudinal stretch is twice the 2 horizontal squishes, so volume is preserved. (Remember, the field lines converge so they don't point in the same direction on opposite sides of low tide).
One can liken this to the (dipole) polarization of an atom in a (vector) field, where the deformation is characterized by the $Y_{l=1}^{m \in (-1,0,1)}$ spherical harmonics.
It's all very geometric.