The equation you have selected is used to estimate the amplification associated with a harmonic load (omega f) in a single degree of freedom system. Your load appears to be a one-time hit; this would not be harmonic - it is an impulse.
I pushed your event (1ms rise, 1ms flat, 1ms fall) through the program's spectrum generator where a time history is broken down into a frequency response spectrum. The resulting DLF at 45 Hz (283 rad/sec) is about 0.56; not the 0.019 produced by your harmonic load equation.
So why doesn't your calculated "DLF" of 0.3415 line up with this 0.56? Keep in mind the point about the "single degree of freedom system". A single degree of freedom system would have all the mass of the system participating in this single (and only) response. Your piping system is not a single degree of freedom system. Your system has several modes of vibration - the textbook modes of a simple cantilever. The great thing about the response spectrum method is that each mode of vibration is independent of (orthogonal to) all the other modes of vibration and each mode can be evaluated alone. (The total system response being the sum of these modal contributions.) But you must keep in mind that only a portion of each node's mass is assigned to each mode of vibration. If you wish to see the TOTAL response to the impulse, you would have to include ALL modes of vibration in the analysis. Fortunately, high frequency modes respond in a rigid manner and these higher responses can be estimated with a static load - BUT only for the remaining nodal masses (the node's mass not associated with the lower modes). This is that missing mass term in the dynamic Control Parameters.
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Dave Diehl