Braden Hancock Brigham Young University B.S. Mechanical Engineering

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Presentation transcript:

Reducing Shock Interactions in a High Pressure Turbine via 3D Aerodynamic Shaping Braden Hancock Brigham Young University B.S. Mechanical Engineering Graduation 2014 Mentor: Dr. John Clark, AIAA “Engineer of the Year” 2012

Motivation The result of High Cycle Fatigue (HCF) failure in a gas turbine engine Failed engine of an Airbus A380-800 As shown by NY Times , 4 Nov 2010

Outline Causes of HCF Failure Method of 3D Aerodynamic Shaping Experimental Results - Benchmark Method of Surface Normal Projections (SNP) Experimental Results - Comparison Conclusions

Unsteady interactions in a high pressure contra-rotating turbine: Shock Reflections reflection surface Unsteady interactions in a high pressure contra-rotating turbine: 1) Unsteady shock/boundary-layer interaction 2) Shock/shear-layer interactions 3) Moving shock/boundary-layer interaction 4) Reflected shocks 5) Shock/shock interaction vane blade oblique shock blade “A decrease in the level of empiricism in [unsteady flows] would be of significant value in the engine development process…” -Greitzer, E. M., Tan, C. S., Wisler, D. C., Adamczyk, J. J., and Strazisar, A. J., 1994. “Unsteady Flows in Turbomachines: Where’s the Beef?,” Unsteady Flows in Aeropropulsion, ASME AD-Vol. 40, pp. 1-11. vane blade reflected shock location Rotation

Shock Reflection Movement Direction of Travel Velocity of Medium Velocity of Medium Shock Wave Reflected Shock Wave

Shock Reflection Movement Direction of Travel Velocity Velocity Shock Wave Reflected Shock Wave

3D Aerodynamic Shaping Upstream vanes Bowed Baseline Reverse-Bowed 5 Tip Root Bowed Baseline Reverse-Bowed 5 100 DFT mag. / Pt inlet Resulting pressure distributions on upstream blades

Engine Orientation Radial Axial Circumferential

3D Aerodynamic Shaping Upstream vanes Bowed Baseline Reverse-Bowed 5 Tip Root Bowed Baseline Reverse-Bowed 5 100 DFT mag. / Pt inlet Resulting pressure distributions on upstream blades

Genetic Algorithm Many chromosomes together describe an individual Initial Generation Many chromosomes together describe an individual .01742 … 0 1 7 4 2 3 5 0 8 1 9 2 6 4 5 … Calculate Fitness .92645 Selection Two successful individuals mate to form new individuals …017423508192645… …017423508187324… Mating …016354071287324… …016354071292645… Mutation Random mutation occurs occasionally New Generation …017423508192645… …017473508192645…

Genetic Algorithm (GA) Data 3D Unsteady RANS Analysis Fitness Criteria 𝑆 𝑝 Proximity of high pressure point to the root Δ𝛷 How spread out in time the peak pressures are 𝑃′ 𝑙𝑜𝑐 Prevent unsteadiness in the trouble spot fitness SP ΔΦ P ′loc 𝑓= (1− 𝑆 𝑝 ) 4 + Δ𝛷 3π + 1− 𝑃′ 𝑙𝑜𝑐 2 Genetic Algorithm (GA) Data Number of Processors 96 Generations 16 Population size 24 Hours of Runtime per Generation 23.3

Results of CFD Analysis The distribution of: a) total static pressure in terms of DFT magnitude b) phase angle in degrees on the blade suction side due to the baseline and optimized vanes: a) b) 5 180⁰ 100 DFT mag. / Pt inlet 100 DFT mag. / Pt inlet , Phase Angle -180⁰ Baseline Bowed Baseline Bowed Pressure Phase Angle

Surface Normal Projections (SNP) Standard Vane Bowed Vane Shock reflections plotted from the pressure side of a downstream vane to the suction side of an upstream blade

Additional Considerations tip root Standard Bowed The relative magnitudes of shock reflections on an upstream blade from a downstream vane An example of the blockage that can occur due to the presence of an adjacent vane in the line of sight of the projecting surface.

Genetic Algorithm Comparison Genetic Algorithm Optimization Genetic Algorithm Comparison CFD Approach SNP Approach Population size 24 48 Generations 16 80 Pitch Change Range 0 - 20 (-100) - 100 Computation Time per Individual 84000 s 6 s Equations 𝐶 𝑟 = ∑ 𝑟 𝑖 𝑚 𝑖 ∑ 𝑚 𝑖 (1) 𝑀=∑ 𝑚 𝑖 (2) 𝑓= (1−𝐶 𝑟 )+(1 −𝑀) 2 (3) Nomenclature 𝐶 𝑟 center of reflection (by span %) 𝑟 𝑖 radial distance of vertex i from root 𝑚 𝑖 magnitude of reflection at vertex i 𝑀 Total magnitude of reflections 𝑓 fitness

Fitness Trends

Center of Reflection

Relative Magnitude of Reflection

Results of Projection Calculations total sum of reflections M = 1.00 M ≈ 1.00 M = 0.01 100% span 48% span 29% span 6% span 0% span Baseline CFD Optimal Normal Projection Optimal 5 100 DFT mag. / Pt inlet

What’s Next? New transonic cascade facility is on-line (2D) Annular-Cascade, HPT Stage, and Stage +1/2 Testing in the Turbine Research Facility (3D)

Conclusions 1) Vane bowing has been shown to be a viable method for redirecting shock waves to regions of the blade where their detrimental effects will be mitigated. 2) Surface normal projections from downstream vanes may be used to estimate the results of shock reflections on upstream blades. Reduction of pressure fluctuations by 2 orders of magnitude Translation of center of reflection by 42% span Baseline Normal Projection 48% span 6% span 3) Including the SNP method in the design of turbine airfoils holds significant advantages over an approach consisting exclusively of CFD simulations. Reduction of computational time per airfoil by 4 orders of magnitude