As a frequent user of the things - but not on buildings, a couple of comments.
Basically you split the SDOF mode of the main structure into two, one in which the mounting point and the TMD mass move in phase (the lower frequency), and one in which they move in antiphase.
The separation of these two new peaks is governed by the ratio of the inertia of the TMD to the modal mass at the mounting point.
Adding damping to the compliance joining the structure to the TMD inertia is how you control (a) the resonant response at each peak and (b) increasing the response on the shoulders of each peak, and between them. It also has some effect on the frequency split. Generally less damping is better than more, at least with rubber.
If you are just trying to add damping to a troublesome resonance then TMDs work well, if you can fit one at a point of high amplitude.
If your excitation is of a broadband (or impulsive) nature and you have a high modal density then you'll need lots of differently tuned TMDs, or a lot of damping. Some machines use untuned mass dampers in that case.
If you change the tune of the spring you can alter the relative height of the two peaks. This is useful if your excitation spectrum rolls off with frequency, which I imagine is quite common with structures (for instance vibrations from roads) - in that case you set the lower peak at a lower response than the upper one.
A simple 2dof excel model of this is the quickest way to study the various interactions, unless you have a great love for equations.
You can damp more than one mode at one location with the same damper - for instance the crankshaft damper on a car can be constructed so as to damp the first torsional and first bending mode of the crank.
I'd just emphasise that life is a lot easier if you can mount them at the point of maximum amplitude.
Cheers
Greg Locock
SIG

lease see FAQ731-376 for tips on how to make the best use of Eng-Tips.