Slagathor
Mechanical
- Jan 6, 2002
- 129
I have rotating equipment (pump) problem I need some help with. We have a close coupled vertically mounted volute pump with a confirmed structural resonance problem.(In one plane the natural frequency is about 11.1 Hz. In the other plane it is 15Hz. During field testing, weight [a 50# sandbag!] was added to the system, and the critical peaks shifted down about 1.5-1.7Hz. This is a classic structural ressonant condition)
The plan to fix the issue is to add weight to the system (likely a thick plate between motor and motor support) to move the critical frequencies down. We will also modify the pump so that it runs at a faster RPM. This will result in moving our operating speed, and natural frequencies away from each other....pretty simple, really.
My question is with regards to creating a "simple" analytical model for this system. We have determined that 90% of the flexibility in this structure is in the pump, backhead and base. The motor support and motor are relatively rigid. As such I want to model the entire base, pump and backhead as a cantaleverd beam, and model the motor and motor base as a rigid lumped mass hung on the end of the beam with the center of mass some distance from the beam end. The motor and motor support mass and dimensions are known in detail. As such, I can tweak the model of the "beam" (pump, base, backhead structure) to agree with the field data obtained. After getting a model that is close, I can then vary the mass of the lumped mass on the end of the beam to estimate how much mass addition is necessary to move the critical.
(I could of course just guess, based on the field data measured when we added 50# to the top of the motor and the wing it....but that could waste a lot of time and money. i would at least like to make an educated guess as to how much mass we add to the system to get the desired effect of shifting the peaks down by 1.7 Hz/100 RPM))
This model does not have to be perfect. Even a 20% error in critical frequency change will only cause an error of 20 RPM.
One approach is:
1. Consider the pump/base/back head beam to be a perfect beam with no mass. There are two loading schemes we must consider:
- Force acting at end of beam: For this case deflection is given by PL^3/3EI
- Moment acting at end of beam: For this case deflection is given by MoL^2/2EI
So my question is how do I take this system and come up with a solution (frequency)? I am sure this will end up as some sort of crazy Partial Diff Eq problem...it's been way too long since I did that stuff. Anyone know where to go from here. If need be I will put a drawing together and email it to illustrate my approach.
Thanks for any help.
The plan to fix the issue is to add weight to the system (likely a thick plate between motor and motor support) to move the critical frequencies down. We will also modify the pump so that it runs at a faster RPM. This will result in moving our operating speed, and natural frequencies away from each other....pretty simple, really.
My question is with regards to creating a "simple" analytical model for this system. We have determined that 90% of the flexibility in this structure is in the pump, backhead and base. The motor support and motor are relatively rigid. As such I want to model the entire base, pump and backhead as a cantaleverd beam, and model the motor and motor base as a rigid lumped mass hung on the end of the beam with the center of mass some distance from the beam end. The motor and motor support mass and dimensions are known in detail. As such, I can tweak the model of the "beam" (pump, base, backhead structure) to agree with the field data obtained. After getting a model that is close, I can then vary the mass of the lumped mass on the end of the beam to estimate how much mass addition is necessary to move the critical.
(I could of course just guess, based on the field data measured when we added 50# to the top of the motor and the wing it....but that could waste a lot of time and money. i would at least like to make an educated guess as to how much mass we add to the system to get the desired effect of shifting the peaks down by 1.7 Hz/100 RPM))
This model does not have to be perfect. Even a 20% error in critical frequency change will only cause an error of 20 RPM.
One approach is:
1. Consider the pump/base/back head beam to be a perfect beam with no mass. There are two loading schemes we must consider:
- Force acting at end of beam: For this case deflection is given by PL^3/3EI
- Moment acting at end of beam: For this case deflection is given by MoL^2/2EI
So my question is how do I take this system and come up with a solution (frequency)? I am sure this will end up as some sort of crazy Partial Diff Eq problem...it's been way too long since I did that stuff. Anyone know where to go from here. If need be I will put a drawing together and email it to illustrate my approach.
Thanks for any help.