13 Venting Requirements
13 Venting Requirements
13 Venting Requirements
and one meter off the pipe surface. Results would be adjusted
using the A-weighting scale to reflect the noise an average person
would perceive.
The most complex feature of the model was the transmission
loss through the downstream pipe wall. Each pipe size has differ-
ent values and numbers of coincident frequencies impacting the
transmission. For example, a 2-inch Schedule 80 pipe, 5.5 mm
(0.218 inch) wall thickness, has six coincident frequencies; an
8-inch Schedule 40 pipe, 8.2 mm (0.322 inch) thickness, has 68 co-
incident frequencies. A typical pipe response is shown in Figure 4.
Features of the theoretical model were first published by Bau-
mann in 1982.7 The Pennsylvania University results were pub-
Figure 3. Control valve noise model and tested configuration. lished by Reethof in 1985.8 The model was used in a draft standard
for Aerodynamic Noise Prediction by ISA in 1982 and circulated
lower velocity jet exiting the trim can be achieved. for preliminary use and critique. The standard included tables
The flow in Figure 2 is directed toward the outside diameter of of pipe transmission loss in one-third octaves from 25 to 20,000
the trim. However, this could be designed to have flow from the Hz for pipe sizes from 1 to 24 inches of three different pipe wall
outside to the center of the trim if needed. To achieve the desired thicknesses for each pipe size and for pipe fluid Mach numbers
flow through the valve, an appropriate number of disk sets are of zero and 0.3. Predicting the noise required the user to make
stacked on top of each other. The flow is then controlled by a valve numerous interpolations and sum the noise for each of the octave
plug moving up or down through the center, exposing or hiding bands. Accuracy for most valves was estimated to be within ±5
flow paths. There have been many variations to this approach dBA. The valves considered in the model had a single pressure drop
throughout the years. trim like that shown in Figure 3. The standard was not applicable
Due to the uncertainty associated with various valve manufactur- to multi-path, multi-stage type trim like that shown in Figure 2.
ers’ noise predictions, the ISA Control Valve Standards Committee The ISA prediction standard caused a lot of confusion because
arranged a research project in 1974. (The Instrument Society of of its complexity and difficulty in carrying out the laborious
America is now the International Society of Automation; Research calculations. This was a period before the personal computer, so
Triangle, NC). most users had to program this procedure on a large mainframe
The project’s objective was to provide control valve users with with limited availability because of other computing demands. As
a single noise prediction method that was based on theoretical a result, the ISA committee made some simplifications by creating
fundamentals of the physical process. Multiple control valve five separate jet Mach number regimes and providing the complex
manufacturers contributed to the research that was conducted by pipe transmission loss functions in a number of representative
Pennsylvania State University.6 The research included testing of a formulations. The first approved standard was published in 1989,
simple valve design (see Figure 3) so that the methodology could be seven years after the first draft.
supported with as few empirical factors as possible. The key factors With this new noise prediction model, the users could calculate
that were established were acoustical efficiency and the amount of an expected noise level, which was frequently different from what
noise generated that exited the valve into the downstream piping. the control valve manufacturers would state. The manufacturers
Acoustical efficiency was on the order of 0.04 percent of the total needed to make adjustments to the model to improve the accuracy
jet kinetic energy, and only one-fourth of the total noise generated for their products to avoid possible warranties associated with not
was typically propagating into the downstream pipe. meeting specification requirements. The prediction differences
The resulting theoretical model for the valve tested consisted were debated, and both parties eventually moved on to other
of four parts: important matters. However, uncertainty still existed, since there
• Calculating total jet kinetic energy exiting the valve pressure was a lack of confidence in the noise prediction methodology.
reducing trim. ISA through its U.S. representative to the International Electro-
• Estimating the amount of this energy that was converted to technical Committee (IEC) urged the Control Valves Subcommittee
acoustical energy. under IEC 65B to adopt the more accurate physics-based noise
• Determining the amount of acoustical energy that was transmit- prediction method. The same confusion caused by each control
ted through the downstream pipe wall. Noise radiated from the valve manufacturer having a different noise prediction method
bulky valve body was considered negligible. also existed on an international level. There was a German Stan-
• Calculating how much of the noise transmitting through the pipe dard, VDMA 24422-1989, for noise prediction, but it relied on a
was radiated to a listener one meter downstream of the valve number of experimental factors that had to be provided by each