The relations for the transformations are fundamentally fixed in variable form regardless of the kinematic theory for how the universe operates, whether it be SR or LET or anything else. Let's say we are stationary in a ship within our own frame and an identical ship passes us in the opposite direction along the x axis, identical in the respect that they measure the same proper length d of their ship as we do of ours. Both ships synchronize the clocks at the front of their ships to T=0 upon passing, when the fronts coincide, which is the origin of each frame. According to our frame, the other ship's clocks are ticking slower by a factor of z, their rulers and ship are length contracted by a factor of L, and they have synchronized so that to us, the clock at the rear of their ship reads a greater time than the front clock by tl, so the other frame is synchronized with an additional time of tl per length L d. An event then occurs according to our frame at coordinates t, x. According to the other frame, the event would occur at x - v t, but their rulers are also contracted, so they measure
x' = (x - v t) / L
The event occurs at time t to us, so when the clock at the front of the other ship reads z t, but the simultaneity difference adds a time tl per length L d in the negative direction also, so the time upon a clock that coincides with the event in the other frame will read
t' = z t - (tl / (L d)) (x - v t)
Those are the fundamental forms of the transformations which would be used regardless of the kinematic theory, so variable with LET. Of course with SR, we have the symmetry principle, whereby z = L = sqrt(1 - (v/c)^2) = 1 / y and tl = z L d v / (c^2 - v^2) = d v / c^2, which gives
x' = y (x - v t)
t' = t / y - (y v / c^2) (x - v t)
= y (t / y^2 - (v / c^2) (x - v t))
= y (t (1 - (v/c)^2) - v x / c^2 + (v/c)^2 t)
= y (t - v x / c^2)