I have not yet seen a problem like this across any course I have taken, but am curious how to approach this. Say that you have a system like this:
Here some torque is being generated at a motor, which causes a shaft to rotate, rotating gear n1, spinning gear n2, which then spins an elastic shaft. This elastic shaft has a fan attached to it, which then rotates at θ_f. I understand this shaft can be thought of as a spring. So we have an additonal term to consider for the equations that govern this system:
K(θ_2-θ_f)
My confusion here lies in deriving a single governing equation. Commonly with a normal non-elastic shaft we could just use a gear ratio say N = n2/n1 in this instance the following are true:
0_m = 0_1, 0_2 = θ_1/N (from gear ratio), θ_2 = θ_f
Thus:
θ_f = θ_m/N
But with this elastic shaft, θ_f does not equal θ-2. How can I account for this?
I thought perhaps a subsition like this:
θ_m = (θ_2 - (θ_f / (n1/n2))) / (1-K/(n1/n2))
might work, but the θ_2 still exists so I cannot fully get an equation in terms of θ_f.
The equations that should govern this system I believe are:
I_m*θ_m'' = T_m - T_1
I_f*θ_f'' = T_2 + K(θ_2-θ_f)
From our gear ratio: T_2 = N*T_1
Is there anyway to directly relate θ_m to θ_f? I figure it would ultimately be a relation between θ_2 and θ_f that makes this possible but I cannot seem to derive it or find anything relevant.
Thank you for your help, it is much appreciated.