Abstract
This paper presents a modeling and computational study on particle erosion in curved ducts. It is found that the average erosion rates per impact range from <path id=x30 d=M241 635q53 0 94 -28.5t63.5 -76t33.5 -102.5t11 -116q0 -58 -11 -112.5t-34 -103.5t-63.5 -78.5t-94.5 -29.5t-95 28t-64.5 75t-34.5 102.5t-11 118.5q0 58 11.5 112.5t34.5 103t64.5 78t95.5 29.5zM238 602q-32 0 -55.5 -25t-35.5 -68t-17.5 -91t-5.5 -105 q0 -76 10 -138.5t37 -107.5t69 -45q32 0 55.5 25t35.5 68.5t17.5 91.5t5.5 105t-5.5 105.5t-18 92t-36 68t-56.5 24.5z /> to <path id=x39 d=M244 635q90 0 143 -72t53 -177q0 -133 -65 -229.5t-171 -139.5q-79 -32 -140 -32l-5 30q109 18 185 91t101 186l-68 -36q-29 -16 -60 -16q-79 0 -129 51.5t-50 130.5q0 80 57 146.5t149 66.5zM228 602q-52 0 -78 -45.5t-26 -98.5q0 -69 36.5 -115.5t97.5 -46.5 q53 0 90 28q4 31 4 66q0 51 -9.5 95.5t-39 80.5t-75.5 36z /> <path id=x35 d=M153 550l-26 -186q79 31 111 31q90 0 141.5 -51t51.5 -119q0 -93 -89 -166q-85 -69 -173 -71q-32 0 -61.5 11.5t-41.5 23.5q-18 17 -17 34q2 16 22 33q14 9 26 -1q61 -50 124 -50q60 0 93 43.5t33 104.5q0 69 -41.5 110t-121.5 41q-53 0 -102 -20l38 305h286l6 -8 l-26 -65h-233z /> <path id=x33 d=M285 378v-2q65 -13 102 -54.5t37 -97.5q0 -57 -30.5 -104.5t-74 -75t-85.5 -42t-72 -14.5q-31 0 -59.5 11t-40.5 23q-19 18 -16 36q1 16 23 33q13 10 24 0q58 -51 124 -51q55 0 88 40t33 112q0 64 -39 96.5t-88 32.5q-29 0 -64 -11l-6 29q77 25 118 57.5t41 84.5 q0 45 -26.5 69.5t-68.5 24.5q-67 0 -120 -79l-20 20l43 63q51 56 127 56h1q66 0 107 -37t41 -95q0 -42 -31 -71q-22 -23 -68 -54z /> mm 3/g under current conditions. For each doubled inlet velocity, the increases of erosion rates per impact are 2–14 times. The erosion rate per impact varies with particle diameter with “ √” shape through bends, which is similar to the particle deposition behavior in duct flows. The erosion rate curves per injected particle show the shapes of a 90-degree anticlockwise rotated “S” and a wide open “V,” respectively, for three larger and smaller inlet velocities. The average erosion rates per injected particle are 1.4–18.9 times those rates per impact due to huge amounts of impacting, especially for those depositing particles. It is obvious that the erosion rate distribution per impact is similar to a “fingerprint” with five clear stripes and a lower “cloud” along the bend deflection angle for the three largest particles; yet, for other smaller particles, the erosion rate distributions are much like an entire “cloud.”
Highlights
Particulate flow is a significant phenomenon in environmental, industrial, medical, and lifetime applications
The airflow and particle flow models were validated by experimental data through previous works [8, 19] in terms of the air and particle velocity profiles, and particle depositions and penetrations, which support the present investigations
This paper presented a modeling and computational study on particle erosion in curved ducts
Summary
Particulate flow is a significant phenomenon in environmental, industrial, medical, and lifetime applications. The aerosol deposition, accumulation, and soiling on solar panels and glazing glass will erode their surfaces obviously [4]. These applications include a large amount of straight and curved duct flow. The particle flow and erosion in bends have not been fully studied [5, 6]. El-Behery et al [7] studied the penetration rate distribution for estimating solid particle erosion in curved 90∘ and 180∘ ducts. Sun et al [8] studied the particle penetration and deposition in and behind bends. Some studies have been conducted to investigate the particle erosion in bends, prediction research on the erosion distribution is limited
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