Transfer function and state space model are developed for torque applied on a mass through gear train.
| (input) | τ1(t) | = | applied torque | |
| (output) | θ1(t) | = | top gear angle | unknowns |
| τ2(t) | = | torque on mass due to τ1 | ||
| θ2(t) | = | mass rotational position | ||
| r1 | = | top gear radius | ||
| r2 | = | bottom gear radius | ||
| J | = | inertia |
3 unknowns so 3 equations are needed. During the process of formulating these equations, a new unknown variable, f(t), is introduced; therefore, a total of 4 equations are prepared.
where f(t) is a new unknown variable which corresponds to the force
applied to the top gear due to the bottom gear.
Force on top gear is applied on bottom gear with equal but
opposite direction (action-reaction). τ2(t) is not
present because it is the same as the torque due to f(t).
If τ2(t) were used instead, f(t) would not be present.
Laplace transform (eq. 1), (eq. 2), (eq. 3), (eq. 4):
Solve for the 4 unknowns:
Solve output/input:
Transfer functions for block diagram is derived using Laplace equations from previous section:
When a mass is present in a system, its position and velocity are commonly chosen as state variables. Similarly for the rotational case, angle and angular velocity are chosen for state variables. It can also be noted that applied torque (input), angle, and angular velocity are sufficient to determine this system's future angle (output). This confirms the selected state variables are valid for this system.
State vector:
Input vector:
Output vector:
Rewrite (eq. 1), (eq. 2), (eq. 3), (eq. 4) in these new notations:
Rearrange equations to express αΊ‹(t) and y(t) in terms of x(t) and u(t):
Rearrange in matrix format: