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Reducing Jet Noise with Chevron Nozzles

Principal Investigator: Matthias Meinke, Chair of Fluid Mechanics and Institute of Aerodynamics (AIA), RWTH Aachen University, Aachen (Germany)
HPC Platform: Hazel Hen of HLRS

Noise reduction is one of the major challenges of today’s aircraft development and together with an increase in fuel efficiency one of the key goals in European aircraft policy. The perceived noise levels of flying aircraft are to be reduced until 2050 by 65% compared to 2000. Various ideas exist to reduce aircraft noise. One of the major noise sources at take-off is the engine jet noise. Recently, serrated or chevron nozzles were introduced, since the flow structures in the jet depend on the details of the nozzle exit geometry and have a large impact on the noise sources in the jet. This kind of passive device has drawn a lot of attention in research and aircraft industry and is also investigated in this project. Figure 1 shows a model for a baseline configuration of an aircraft engine nozzle and a chevron nozzle.

Reducing Jet Noise with Chevron NozzlesFigure 1: Model of a baseline nozzle (left) and a chevron nozzle (right).
Copyright: AIA, RWTH Aachen University

A major problem of chevrons is, that while they can lead to a noise reduction during aircraft take-off, this nozzle design can, however, also lead to a severe loss of thrust during both take-off and cruise flight and thus to a lower efficiency of the engine. In addition, the noise reduction of chevrons can be intricate. They can reduce low frequency noise at large aft angles but at the same time increase high frequency noise at sideline angles.

These two aspects lead to a shape-optimization problem for the chevron nozzle design with the goal of reducing the low-frequency noise under the constraint of avoiding thrust reduction and an increase in high-frequency noise. For the shape optimization the influence of several design parameters, like the number of chevrons, penetration angles and the chevron length should be investigated.

High-performance computing (HPC) can help to tackle these research questions in a multi-stage process. In the first step, the unsteady compressible flow field of the jet is computed by using a so-called large-eddy simulation. In a second step, acoustic sources are determined from the flow field and acoustic perturbation equations are solved to determine the noise generation and propagation, i.e. the resulting acoustic sound field. With an optimization strategy, the nozzle design will be modified with the goal of noise reduction while maintaining the thrust of the engine.

The correct prediction of the jet noise, i.e. pressure waves of small amplitude, requires an accurate simulation of the flow field. This can only be achieved with simulations based on a highly resolved mesh with up to 1 billion mesh cells, since the fully turbulent flow field contains a broad range of scale lengths. To conduct such simulations, efficient, memory optimized and fully parallelized algorithms are required, that are adapted to high-performance computing hardware such as the Hazel Hen supercomputer installed at HLRS.

Reducing Jet Noise with Chevron NozzlesFigure 2: Turbulent kinetic energy distribution for a baseline nozzle (top) and a chevron model (bottom).
Copyright: AIA, RWTH Aachen University

The effect of the chevron nozzles on the flow field can be seen in Figure 2. Here, the turbulent kinetic energy of two jets, exhausting from a circular baseline and a chevron nozzle, is visualized. As it can be seen in Figure 2, chevrons obviously enhance the mixing process. This weakens the formation of large-scale structures and excites smaller scale structures. Smaller turbulent scales are associated with high-frequency noise generation and large-scale structures to low-frequency noise.

Reducing Jet Noise with Chevron NozzlesFigure 3: Temperature field of a jet emanating from a coaxial chevron nozzle.
Copyright: AIA, RWTH Aachen University

Figure 3 shows contours of constant Mach number, coloured by the temperature of the flow field. The small-scale turbulent structures are clearly visible in the mixing layers of the jet.

Reducing Jet Noise with Chevron NozzlesFigure 4: Sound field generated by the jet flow.
Copyright: AIA, RWTH Aachen University

Figure 4 shows sound waves that are generated in the jet flow and propagate into the far field, which shows the preferred sound propagation at an angle of about 30o – 40o relative to the axis of the main flow direction. In the next steps an optimization for the chevron geometry will be performed using the computational resources of HazelHen.

Project Team:

Matthias Meinke (PI), Vitali Pauz, Wolfgang Schröder
Chair of Fluid Mechanics and Institute of Aerodynamics, RWTH Aachen University

Scientific Contact:

Chair of Fluid Mechanics and Institute of Aerodynamics
RWTH Aachen University
Wüllnerstr. 5a, D-52062 Aachen (Germany)
email: m.meinke [at] aia.rwth-aachen.de
http://www.aia.rwth-aachen.de

April 2017

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