EsportToys
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Joined 4 years ago
And obviously it would only apply for the underdamped case.
And even if you are to calculate the integration factors based on dynamic frame rates, they only need to be computed just once per frame for all objects that share the same damping configuration.
m * x’’ + c * x’ + k * x = f(t)
See https://web.archive.org/web/20230604215211/https://esporttoy...https://www.desmos.com/calculator/mu80ttc9aa
function sprung_response(t,pos,vel,k,c,m)
local decay = c/2/m
local omega = math.sqrt(k/m)
local resid = decay*decay-omega*omega
local scale = math.sqrt(math.abs(resid))
local T1,T0 = t , 1
if resid<0 then
T1,T0 = math.sin( scale*t)/scale , math.cos( scale*t)
elseif resid>0 then
T1,T0 = math.sinh(scale*t)/scale , math.cosh(scale*t)
end
local dissipation = math.exp(-decay*t)
local evolved_pos = dissipation*( pos*(T0+T1*decay) + vel*( T1 ) )
local evolved_vel = dissipation*( pos*(-T1*omega^2) + vel*(T0-T1*decay) )
return evolved_pos , evolved_vel
end
For anticipation, just add an extra initial velocity in the opposite direction and let the closed-form solution handle the time evolution. The main trick here is to keep both position and velocity as state. There is no need to “step through the simulation”.The following is the complete solution in Lua:
function sprung_response(t,pos,vel,k,c,m)
local decay = c/2/m
local omega = math.sqrt(k/m)
local resid = decay*decay-omega*omega
local scale = math.sqrt(math.abs(resid))
local T1,T0 = t , 1
if resid<0 then
T1,T0 = math.sin( scale*t)/scale , math.cos( scale*t)
elseif resid>0 then
T1,T0 = math.sinh(scale*t)/scale , math.cosh(scale*t)
end
local dissipation = math.exp(-decay*t)
local evolved_pos = dissipation*( pos*(T0+T1*decay) + vel*( T1 ) )
local evolved_vel = dissipation*( pos*(-T1*omega^2) + vel*(T0-T1*decay) )
return evolved_pos , evolved_vel
end
[0] https://esporttoys.pages.dev/2022/11/21/damped
https://github.com/esporttoys/librescroll