Turbine Aerothermodynamics Laboratory - Facilities
Facilities
The low-speed windtunnel at the ARC (Fig. 1) is a blower type tunnel which features two test sections (each 0.38m x 0.38m). Included is the capability of increasing free-stream turbulence levels as high as 12% and a built in heater to be used for heat transfer applications. A variety of experimental studies have been performed on this facility covering the topics of boundary-layer interactions with free-stream turbulence and surface roughness, film-cooling effectiveness, and applications of active flow control to boundary layer separation and secondary flows. The tunnel is capable of velocities up to 30 m/s with free-stream turbulence levels less than 0.4% in a clean configuration.
Flow diagnostic capabilities include two- and three-component particle image velocimetry, infrared thermography, single- and double-element hot-film anemometry, and a variety of pressure transducers and probes including a bank of 32 pressure transducers that can be used to obtain rapid measurements of airfoil pressure distributions. Flow visualization using smoke wires, tufts, and oil have been used in the past.
The transonic wind tunnel is a blowdown facility with a cross section of 6” wide by 22” high (0.15x0.56 m) and a test section length of 44” (1.12m), with optical access from the top and both sides. The settling chamber contains a perforated plate, honeycomb and eight screens (60-mesh) used to improve flow quality, resulting in a turbulence level of +/- 0.5%. Within the test section, perforated sidewalls with 1/8” holes (6% porosity) create isolated cavities for reducing Mach wave reflections, and a cam mechanism can articulate the test article at controlled frequencies up to 25 Hz. The Reynolds number and Mach number can be independently set according to test specifications. Reynolds numbers can range from 2 to 16 million per foot of chord, while a steady freestream Mach number can range from 0.18 to 1. In addition to steady freestream Mach numbers, the tunnel is capable of producing Mach number oscillations, independent or phase-locked to those of the test article, with an amplitude of 0.07.
This facility has been used to examine an airfoil under isolated variations in Mach number and angle of attack. Recently, an investigation of coupled oscillations in Mach and angle of attack, simulating a helicopter in forward flight, has been conducted. Flow control of the test article has also been investigated using vortex generator jets (VGJs) and nanosecond pulsed Dielectric Barrier Discharge (NS-DBD) actuators.
Tunnel Instrumentation includes:
- Kilohertz test article surface pressure measurements
- Traversing wake probe total pressure measurements
- Angle of attack, phase, and Mach oscillation angles
- Thermocouple and thermistor temperature measurements
- Optical access for Particle Image Velocimetry (PIV) and Pressure Sensitive Paint (PSP)
- Hundred-kilohertz total and static tunnel pressure transducer measurements
Internal Deposition Facilities
In modern gas turbine engines, one of the most common methods used to cool components is to employ a double-wall cooling configuration. This method, typically used for turbine vane and blade cooling, utilizes a combination of impinging jets, through-wall flow, and film cooling to reduce metal temperatures to acceptable levels. Because of the complex nature of these flows, they are susceptible to particulate deposition that reduces the cooling effectiveness of the coolant flow, potentially leading to part failure. At the Turbine Aerothermodynamics Laboratory, a simplified double-wall test article (shown below) is used to evaluate the effects of numerous parameters on the buildup of particulate and subsequent flow blockage development.
Heated flow can be supplied to the test article, which can be placed inside an electric kiln to generate representative metal temperatures. Particulate is delivered to the article via a conveyor system, allowing for precise control over the rate of particle injection. This facility has been instrumental in making several unique discoveries. The most important of these is that the mechanisms responsible for deposition are independent of the rate of particle ingestion, which validates the use of accelerated testing in laboratory environments. Another key observation was the discrete effects small particles have versus larger particles. As shown in the plot below, it was demonstrated that small particles (less than 3 microns) were primarily responsible for deposit buildup, while larger particles (greater than 5 microns) were actually capable of removing existing deposit and limiting the rate of deposit growth. Such information is very beneficial for the purposes of modeling deposition behavior.
A schematic of the more small-scale internal deposition testing facility is shown in the image below. The test section portion is modular, allowing for various other cooling geometries to be studied such as effusion cooling common in combustor liners. The flow can be heated either with the use of an in-line heater or by utilizing electric heating tape wraps depending upon the desired temperature range for a given experiment.
High Pressure Facility
Outside of full engine testing, very few facilities have the capability of running at elevated pressures, let alone pressures representative of the overall pressure ratio of an aero engine. The TuRFR and internal deposition facilities exhaust to ambient pressure. In these facilities, cooling geometry mechanisms are operated by matching the pressure ratio and fluid temperatures which therefore means Mach number is matched. However, since the absolute pressure is not matched, these test facilities operate with a substantially lower fluid density than in an actual engine. This has direct implications to particle deposition testing. Higher fluid density means higher particle Reynolds numbers which in turn yields a lower effective Stokes number. The Stokes number describes the ability of a particle to follow flow streamlines; a Stokes number St<<1 implies the particle follows the streamlines well, while a Stokes number St>>1 implies the particle follows a more ballistic trajectory. In addition, higher density flow yields greater wall shear stress and heat transfer which effect particle sticking mechanics.
In an effort to study the effects pressure has on particle deposition, a high-pressure test facility was constructed for the Turbine Aerothermodynamics Laboratory at the ARC. Shown in the schematic below, the facility is capable of operating at up to 18 atmospheres and flow temperature up to 1,200 °F and is used to study deposit formation on an impingement plate test coupon. Testing has found that deposition at higher pressure changes the deposit structure as well as reduces the volume of captured deposit.
Coefficient of Restitution Facility
One of the primary goals of current particle deposition research is to develop a physics-based model that, in conjunction with a fluid flow solver, can be used to accurately predict the deposition and rebound behavior of particles in gas turbine environments. Unfortunately, existing physical models for the impact mechanics of particles require mechanical property information about the particulate that is unavailable. The Coefficient of Restitution Test Facility at the Turbine Aerothermodynamics Laboratory, shown below, is designed to provide this information by examining the rebound characteristics of particulate over a wide range of parameters, including velocity, impact angle, flow temperature, and surface temperature.
Particle shadows are recorded with a high speed camera as the particles impact the target surface, as shown in the image below. The images are subsequently processed using an in-house code, yielding trajectory information both pre- and post-impact, as well as size and shape information for each identified particle. The quantity of data generated (around 500-600 thousand rebounds per test series) allows for in-depth statistical analyses of the relative effects of different parameters. This information can then be used as an input to a deposition model by means of generating mechanical properties as a function of temperature, for example.
nitored upstream and downstream of the test section by wall static pressure taps. A traverse placed downstream of the test section and moving parallel to the cascade exit plane allows for wake surveys to be taken. A row of choke bars is located in the test section exit duct. These are used to set the area ratio based on the number and diameter of bars, and thus set the Mach number during choked flow. The inlet Mach number can be varied from 0.11 to 0.44. The Reynolds number is set by altering stagnation pressure. The range of possible Reynolds number is broadened by running an ejector sealed at the tunnel exhaust with two stages of axisymmetric nozzles. By lowering the exhaust pressure, the ejector allows decreasing the Reynolds number while maintaining choked conditions.
The facility has recently been utilized to study the use of flow control by means of vortex generating jets on a highly loaded low pressure turbine blade. This study has examined the effects of compressibility and the losses associated with the presence of shock waves and shock-induced separation. Also examined was the effect of surface roughness on the flow field and control performance. Measurements of Cp and Mach distribution along the blade profile are made via static pressure taps on the blades. A Kiel probe traverse at the exit of the blade passage is used to study the total pressure loss in the wake. Shadowgraph is utilized to observe the shock in the cascade center passage by means of a parallel light source and a high speed CMOS camera. Pressure sensitive paint (PSP) is applied to a blade in order to visualize the three-dimensional flow effects brought on by the vortex generating jets.
Transonic Cascade for Nozzle Guide Vane (NGV)
A new transonic linear cascade has been recently commissioned at the Ohio State University (OSU) Turbine Aero-thermodynamics Lab to study film cooling on nozzle guide vane (NGV). The transonic cascade facility consists of a supply plenum and a test section. The tunnel operates in a blow-down mode using a high pressure air supply reservoir (21m3 at 16Mpa) and exhausts to ambient. The plenum section is made out of 37.5mm aluminum plate. High pressure supply air flows into a 155mm x 500mm calming section where it is conditioned for flow uniformity by honeycomb screens. The flow is then accelerated into the 100mm x 250mm test section by a 3:1 contraction. The tunnel is designed to run up to one minute at a maximum massflow rate of 3.25 kg/s. The side walls of the test section are made out of 25mm thick aluminum plate and the end walls are made out of 25mm thick acrylic plate for maximum optical access. The test section includes a rectangular cascade inlet section and a vane passage section followed by an adjustable turning section.
A total pressure Kiel probe and a J-type thermocouple are used to measure the upstream stagnation pressure and temperature. A turbulence grid was used two chords (2C) upstream of the vane leading edge to generate freestream turbulence. A row of static pressure taps is used to measure the upstream static pressure and upstream Mach number. The upstream static pressure taps are placed 1C upstream of the vane leading edge and five taps are used to estimate inlet flow uniformity. The vane passage section includes three vanes-two full passages and two half passages. The curvature of the side walls in the vane-passage section was determined using CFD results performed for an infinite cascade. Three vanes are used to ensure a periodic flow at the central vane for heat transfer study. Two IR viewports are used to measure the surface temperature of different sections of the vane. The IR viewport at the turning section was used to measure the surface temperature of the suction surface of the vane. The turning section consists of two tailboards that can be adjusted independently. There are five static pressure taps at 0.25C downstream of the vane trailing edge to measure the exit Mach number. The tailboard can be adjusted by a set-screw that is connected to a connecting rod. Three connecting rods are used as a support structure and to adjust both tailboards. In addition, a slot was made to place a total pressure Kiel probe at 0.25C downstream of the vane trailing edge to measure the exit total pressure. This pressure measurement is used to estimate the total pressure loss due to film cooling.
The demand for higher fuel efficiency and reduced noise continues to push the trend of increasingly larger bypass ratio turbofan engines with increasingly higher turbine inlet temperature. These trends in aircraft propulsion have levied increasing demands on the turbine (hot) section of modern turbofan engines and on the low-pressure turbine efficiency and work output. Additionally, growth markets for turbofan engines have moved from North America and Europe to the Middle and Far East. Air quality concerns in these new markets are presenting increasing hardship for turbines as airborne deposits collect in cooling passages in the gas turbine and reduce performance. A turbine accelerated deposition facility was commissioned to address the issue of harsh operating environments and high temperature.
A unique Turbine Reacting Flow Rig (TuRFR) was constructed for the Turbine Aerothermodynamics Laboratory at the ARC in 2008 that simulates the flow exiting a gas turbine combustor as it impacts the first stage turbine nozzle guide vanes (NGVs). This early facility is capable of providing main gas path flow temperatures up to 2,100° F with an inlet Mach number of 0.1 and coolant temperatures up to 1,000° F. Airborne particulate can be added to the main gas path and/or the coolant flow to simulate in an experimental environment the deposition build-up observed on NGVs in the field. The spatial temperature distribution in the inlet plane can be modified to simulate various pattern factors typical of modern engines. Optical access allows for video footage of deposition growth as well as surface temperature measurement with infrared imaging. Temperature, velocity, and pressure probes can be traversed across both the inlet and exit planes.
Design and construction of an upgraded and world class “TuRFR II” facility was completed in the summer of 2015 representing a $2M infrastructure investment at the ARC. This impressive facility simulates a more modern engine environment, capable of operating at significantly higher temperatures and mass flow rates. An industrial burner, capable of temperatures up to 3,000° F, provides heated airflow to the NGVs downstream. A double walled construction with liner cooling permits the test section to operate in excess of 2,600° F while internal cooling airflow to the engine parts is provided at up to 1,200° F. TuRFR II shares the testing capabilities of its predecessor, including: particulate injection options, inlet flow pattern factor variations, optical access for infrared thermography, and inlet and exit plane instrumented traverse access. The modular nozzle box test section allows for experiments to be designed for a large array of current engine nozzle guide vane hardware. The TuRFR II facility is employed in exciting research sponsored by various industry leaders.