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Sub-modeling Approach for Large Systems



Although I'll reiterate here you DO NOT need to use the model developed from Problem 6.1 (on the last homework) at all to complete Problem 7.1, it's worth making a few comments about attack strategies for larger systems (described by several/many equations in a problem statement).

Below is a block diagram for the hydraulic servomechanism described in 6.1:

You should understand both how to use/extract sub-parts of a big system and how to create a larger system from individual sub-parts.

The first key idea that will help you is that each block of the diagram represents some specific transfer function of its own. Various particular groups of blocks also represent transfer functions. You may be asked for the transfer function from e_ref to theta_t, but along the way, you can also obtain the transfer function from (for instance) i [current] to omega_t (angular velocity). Below is the sub-part of the total system representing the transfer function (omega_t(s))/(i(s)):

...which can be simplified(?) to become... ("simplified" in that it's more clearly just a first-order system)

"OK, I guess I get that idea," you say, "but how the heck would you ever figure out the that big system at the top in the first place??"

Funny you should ask, because that's the second key idea: "a mountain is climbed one step at a time." Yeah, that sounds cliche, but I really do think it's good advice. Avoid panic. :^) Build up larger transfer functions from smaller sub-units. For instance, with Problem 6.1, you can start by finding each of the following and then linking them up. A general strategy is that after you start with some arbitrary block, you NEXT generally solve for some block that will link up to either the input or output of what you currently have.
Then, you make some educated guess about the inertia-damping-spring system needed to represent the rotating table and roller bearings. (I assumed just inertia and damping here.)
This would allow you to relate the feedback transfer function from omega_t to T_t (torque at table):

...and then the relationship from T_t to P comes from a balance of POWER:

From here, we integrate each side and then reduce everything by using various relationships given in the problem statement:


All that said, this problem was not trivial and did rely on intuition about the spring-mass-damping characteristics of the table [you could test which elements would result in the desired first-order response specified in the statement to figure out if the spring and/or damping was necessary]; the POWER BALANCE step; and careful stepping through each of the relationship given in the problem statement.

You can go through all these steps by manipulating the equations directly, without ever using 'block diagrams', but I find think block diagrams to be a great visual aide.
gonzo@mit.edu page 2 (of 10) 2.010 Tutorial #7, 5-Nov-00