Consider two electrons in an entangled state such as this one:
$$|\psi\rangle = \frac{1}{\sqrt{2}}(|p_x,\uparrow\rangle |-p_x,\downarrow\rangle - |p_x,\downarrow\rangle |-p_x,\uparrow\rangle)$$
That is, the electrons leave a source with opposite momenta $p_x,-p_x$, and when the particle traveling "left" (with negative momentum in the x direction $-p_x$) has spin up ($\uparrow$), then the particle travelling "right" (with positive x-momentum $p_x$) has spin down ($\downarrow$). Similarly when the particle traveling left has spin down, the particle traveling right has spin up. Easy peasy, right?
Now imagine you put two Stern-Gerlach magnets in oposite directions in the way of the beams of electrons emerging from the experiment. Stern-Gerlach magnets scatter the electron up if the spin is up, and down if the spin is down. In quantum mechanics this is straightforward, this is a measurement that will yield probabilities given by the Born rule. We just need to know one particle goes up, the other one goes down. It turns out like this no matter in which order the particles enter the magnets and undergo the interaction/measurement. This applies always and is a tested prediction of quantum mechanics.
However, in Bohmian mechanics there is an issue. There one tries to construct a piloting wave that interacts with the Stern-Gerlach magnet and then guides the particle. However, it turns out that one cannot make the guiding wave only a function of the position of just one of the two electrons!
To understand this, imagine the Stern-Gerlach magnet on the left is a bit further so that the electron traveling with momentum $p_x$ enters the Stern-Gerlach device on the right earlier. It goes "up" or "down" as a random process as determined by the potential generated by the guiding wave. But what about the electron on the left? It has to go in the opposite direction once entering the Stern-Gerlach magnet! Its guiding wave has been determined by the fate of the electron on the right. This turns out to be an instantaneous effect that travels faster than light.
Without going into technical details, this is the property that breaks the whole idea of Bohmian mechanics of constructing a nice local potential that guides your particle through nice local interactions. When entanglement is introduced, there necessarily has to be "spooky action at a distance" in the equations of Bohmian mechanics that is about as weird as quantum mechanics on its own. (This is also the reason why the droplet analogue of Bohmian mechanics will never be able to describe entanglement.)