Mq¨+Cq˙+G(q)+K(q−θ)Jmθ¨+Bmθ˙−K(q−θ)=0(1) link dynamic=τm(2) motor dynamic
The transmitted elastic torque:
τc=K(θ−q)
So we simplify this system to:
q¨=M−1(τc−Cq˙−G(q))
θ¨=Jm−1(τm−τc−Bmθ˙)
Compute the second derivative of τc:
τ˙c=K(θ˙−q˙)
τ¨c=K(θ¨−q¨)
τ¨c=K[Jm−1(τm−τc−Bmθ˙)−M−1(τc−Cq˙−G(q))]
link-side motion appears in the torque dynamics:
τ¨c+K(Jm−1+M−1)τc=KJm−1τm−KJm−1Bmθ˙+KM−1(Cq˙+G(q))
τ¨c+K(Jm−1+M−1)τc=KJm−1τm−KJm−1Bmθ˙+KM−1(Cq˙+G(q))
so the function becomes:
(Jm−1+M−1)τc=Jm−1τm−Jm−1Bmθ˙+M−1(Cq˙+G(q))
at the same time, as there is no deformation, the movement of the motor and the link is completely synchronised θ=q,θ˙=q˙,θ¨=q¨.
(Mq¨+Jmθ¨)+Cq˙+Bmθ˙+G(q)=τm
(M+Jm)q¨+(C+Bm)q˙+G(q)=τm
from the torque dynamics above, K→0, then
τ¨c=0⟹τc=0
From the :
Mq¨+Cq˙+G(q)Jmθ¨+Bmθ˙=0link side=τmmotor side
The motor and the connecting rod are completely decoupled. The torque cannot be transmitted to the connecting link side (τc=0) because the intermediate medium is too soft. The connecting link will simply drop straight down under its own weight, whilst the motor spins idly at the other end.