However, here I have example solutions of one equation using default and "Backward Difference Formula" of order 1 (i.e. Implicit Euler) Method. As we will see later, the "default" method in this case is "Backward Difference" of higher order.
eqn=-u0 \[Omega]^2 Sin[t \[Omega]] + (g x[t])/r + 2 b x'[t] + x''[t];
vals = {b -> 0.001, r -> 0.42578125, g -> 9.81, u0 -> 0.01};
ns1 = NDSolve[{0 == eqn /. vals /. \[Omega] -> 3.14,
x[0] == 0.001, x'[0] == 0.001}, x, {t, 0, 200}][[1]];
ns2 = NDSolve[{0 == eqn /. vals /. \[Omega] -> 3.14,
x[0] == 0.001, x'[0] == 0.001}, x, {t, 0, 200},
Method -> {"BDF", "MaxDifferenceOrder" -> 1}, MaxSteps -> 10^6,
PrecisionGoal -> 5, AccuracyGoal -> Automatic][[1]]
Plot[{x[t] /. ns1, x[t] /. ns2}, {t, 100, 120}, AspectRatio -> 1/5,
ImageSize -> 800, PlotStyle -> {Green,Red}]
Here is the result: green is the default solution, red is the 1st order BDF.
I have a similar plot, where the blue and red curves come from numerical solutions using gsl routines implementing so called Gear's stepping method:
gsl_odeiv_step_gear1 and gsl_odeiv_step_gear2 (it seems, that the current version of gsl has abandoned these routines, it uses gsl_odeiv2_step_msbdf instead, see docs). Blue is the second order solution (together with points of accepted solution), red is the fisrt order solution (there was too many small steps to show them). The green line of the "default" Mathematica solution line hides behind the blue "gear2" curve.


