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AIM: To create a 3D model of a flow bench and run flow analysis. OBJECTIVES : To obtain a plot of valve lift versus mass flow rate. Find the effect of valve lift on the mass flow rate. To run a parametric study for various valve lift. INTRODUCTION : An airflow bench is a device used for testing…
Sourabh Lakhera
updated on 17 Jul 2020
AIM: To create a 3D model of a flow bench and run flow analysis.
OBJECTIVES :
INTRODUCTION :
An airflow bench is a device used for testing the internal aerodynamic qualities of an engine component and is related to the more familiar wind tunnel. It is used primarily for testing the intake and exhaust ports of cylinder heads of internal combustion engines. It is also used to test the flow capabilities of any component such as air filters, carburetors, manifolds, or any other part that is required to flow gas. A flow bench is one of the primary tools of high-performance engine builders, and porting cylinder heads would be strictly hit or miss without it.
A flow bench consists of an air pump of some sort, a metering element, pressure and temperature measuring instruments such as manometers, and various controls. The test piece is attached in series with the pump and measuring element and air is pumped through the whole system. Therefore, all the air passing through the metering element also passes through the test piece. Because the volume flow rate through the metering element is known and the flow through the test piece is the same, it is also known. The mass flow rate can be calculated using the known pressure and temperature data to calculate air densities and multiplying by the volume flow rate.
Airflow conditions must be measured at two locations, across the test piece, and across the metering element. The pressure difference across the test piece allows the standardization of tests from one to another. The pressure across the metering element allows calculation of the actual flow through the whole system. The pressure across the test piece is typically measured with a U tube manometer while, for increased sensitivity and accuracy, the pressure difference across the metering element is measured with an inclined manometer. One end of each manometer is connected to its respective plenum chamber while the other is open to the atmosphere.
Ordinarily, all flow bench manometers measure in inches of water although the inclined manometer's scale is usually replaced with a logarithmic scale reading in the percentage of the total flow of the selected metering element which makes flow calculation simpler. The temperature must also be accounted for because the air pump will heat the air passing through it making the air downstream of it less dense and more viscous. This difference must be corrected for. Temperature is measured at the test piece plenum and at the metering element plenum. Correction factors are then applied during flow calculations. Some flow bench designs place the air pump after the metering element so that heating by the air pump is not as large a concern. Additional manometers can be installed for use with handheld probes, which are used to explore local flow conditions in the port.
The airflow bench can give a wealth of data about the characteristics of a cylinder head or whatever part is tested. The result of the main interest is bulk flow. It is the volume of air that flows through the port in a given time. Expressed in cubic feet per minute or cubic meters per second/minute. Valve lift can be expressed as an actual dimension in decimal inches or mm. It can also be specified as a ratio between a characteristic diameter and the lift L/D. Most often used is the valve head diameter. Normally engines have an L/D ratio from 0 up to a maximum of 0.35. For example, a 1-inch-diameter (25 mm) valve would be lifted a maximum of 0.350 inches. During flow testing, the valve would be set at L/D 0.05 0.1 0.15 0.2 0.25 0.3 and readings taken successively. This allows the comparison of efficiencies of ports with other valve sizes, as the valve lift is proportional rather than absolute. For comparison with tests by others, the characteristic diameter used to determine lift must be the same.
Flow coefficients are determined by comparing the actual flow of a test piece to the theoretical flow of a perfect orifice of equal area. Thus the flow coefficient should be a close measure of efficiency. It cannot be exact because the L/D does not indicate the actual minimum size of the duct. Using extra instrumentation (manometers and probes) the detailed flow through the port can be mapped by measuring multiple points within the port with probes. Using these tools, the velocity profile throughout the port can be mapped which gives insight into what the port is doing and what might be done to improve it. Of less interest is mass flow per minute or second since the test is not of a running engine that would be affected by it. It is the weight of air that flows through the port in a given time. Expressed in pounds per minute/hour or kilograms per second/minute. Mass flow is derived from the volume flow result to which a density correction is applied.
With the information gathered on the flow bench, the engine power curve and system dynamics can be roughly estimated by applying various formulae. With the advent of accurate engine simulation software, however, it is much more useful to use flow data to create an engine model for a simulator.
PROCEDURE :
Inlet Valve position variation [in m] | 0.001 | 0.001 | 0.001 | 0.002 | 0.002 | 0.002 | 0.003 | 0.003 | 0.003 | 0.004 | 0.004 | 0.004 | 0.005 | 0.005 | 0.005 | 0.006 | 0.006 | 0.006 | 0.007 | 0.007 | 0.007 | 0.008 | 0.008 | 0.008 | 0.009 | 0.009 | 0.009 | 0.01 | 0.01 | 0.01 |
Level of initial mesh (Automatic Mesh) | 3 | 4 | 5 | 3 | 4 | 5 | 3 | 4 | 5 | 3 | 4 | 5 | 3 | 4 | 5 | 3 | 4 | 5 | 3 | 4 | 5 | 3 | 4 | 5 | 3 | 4 | 5 | 3 | 4 | 5 |
GG Mass Flow Rate 1 [kg/s] | 2.52527E-06 | -3.67607E-06 | -8.42022E-06 | 1.27446E-05 | -5.09202E-06 | -7.91962E-05 | -4.49153E-05 | -0.000297672 | -0.000140751 | -5.89067E-05 | 0.000209563 | 7.30458E-06 | -0.000253084 | -0.00011077 | -0.000129426 | -0.000113417 | -0.000134424 | -6.76976E-05 | -0.000144718 | -0.000957822 | -0.000284876 | -0.00049109 | -0.001441924 | -0.00098571 | -0.000480029 | -0.001196832 | -0.001192428 | -0.000613238 | -0.001441148 | 5.01411E-05 |
SG Mass Flow Rate 1 [kg/s] | -0.053230398 | -0.050647492 | -0.038160531 | -0.084516206 | -0.078703653 | -0.069192505 | -0.107172947 | -0.10133999 | -0.091720838 | -0.124256106 | -0.118375167 | -0.110325871 | -0.135736492 | -0.129548853 | -0.124126501 | -0.140638227 | -0.137231107 | -0.132586186 | -0.142044404 | -0.140024885 | -0.137146546 | -0.142442355 | -0.140646537 | -0.139816292 | -0.142381073 | -0.140298044 | -0.140224186 | -0.142462396 | -0.140513464 | -0.138689513 |
RESULTS :
Here mass flow rate was the surface goal from outlet of flow bench. Negative sign indicates that mass is leaving the control volume and is just sign convention. For plotting graph between valve lift and mass flow rate this negative sign is removed.
CONCLUSION :
REFERENCES :
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