{"id":{"repo_id":"uno","oai_identifier":"oai:scholarworks.uno.edu:td-2494"},"canonical_url":"https://search.dev.ndltd.org/etd/uno/oai:scholarworks.uno.edu:td-2494","repository":{"repo_id":"uno","name":"University of New Orleans","base_url":"https://scholarworks.uno.edu/do/oai/"},"display":{"title":"An Investigation of Mist/Air Film Cooling with Application to Gas Turbine Airfoils","abstract":"<p>Film cooling is a cooling technique widely used in high-performance gas turbines</p> <p>to protect turbine airfoils from being damaged by hot flue gases. Film injection holes are</p> <p>placed in the body of the airfoil to allow coolant to pass from the internal cavity to the</p> <p>external surface. The ejection of coolant gas results in a layer or “film” of coolant gas</p> <p>flowing along the external surface of the airfoil.</p> <p>In this study, a new cooling scheme, mist/air film cooling is proposed and</p> <p>investigated through experiments. Small amount of tiny water droplets with an average</p> <p>diameter about 7 μm (mist) is injected into the cooling air to enhance the cooling</p> <p>performance. A wind tunnel system and test facilities were build. A Phase Doppler</p> <p>Particle Analyzer (PDPA) system is employed to measure droplet size, velocity and</p> <p>turbulence. Infrared camera and thermocouples are both used for temperature</p> <p>measurements.</p> <p>Mist film cooling performance is evaluated and compared against air-only film</p> <p>cooling in terms of adiabatic film cooling effectiveness and film coverage. Experimental</p> <p>results show that for blowing ratio M=0.6, net enhancement in adiabatic cooling</p> <p>effectiveness can reach 190% locally and 128% overall along the centerline. The general</p> <p>pattern of adiabatic cooling effectiveness distribution of the mist case is similar to that of</p> <p>the air-only case with the peak at about the same location.</p> <p>The concept of Film Decay Length (FDL) is proposed to quantitatively evaluate</p> <p>how well the coolant film covers the blade surface. Application of mist in the M=0.6</p> <p>condition is apparently superior to the M=1.0 and 1.4 cases due to the higher overall</p> <p>cooling enhancement, the much longer FDL, and wider and longer film cooling coverage</p> <p>area.</p> <p>Based on droplet measurements through PDPA, a profile describing how the airmist</p> <p>coolant jet flow spreads and eventually blends into the hot main flow is proposed. A</p> <p>sketch based on the proposed profile is provided. This profile is found to be well</p> <p>supported by the measurement results of Turbulent Reynolds Stress. The location where</p> <p>a higher magnitude of Turbulent Reynolds Stress exists, which indicates higher strength</p> <p>of turbulent mixing effect, is found to be in the close neighborhood of the edge of the</p> <p>coolant film envelope. Also the separation between the mist droplets layer and the</p> <p>coolant air film is identified through the measurements. In other words, large droplets</p> <p>penetrate through the air coolant film layer and travel further over into the main flow.</p> <p>Based on the proposed air-mist film profile, the heat transfer results are reexamined.</p> <p>It is found that the location of optimum cooling effect is coincident with the</p> <p>starting point where the air-mist coolant starts to bend towards the surface. Thus the data</p> <p>suggests that the “bending back” film pattern is critical in keeping the mist droplets close</p> <p>to the surface which improves the cooling effectiveness for mist cooling.</p>","abstract_html":"&lt;p&gt;Film cooling is a cooling technique widely used in high-performance gas turbines&lt;/p&gt; &lt;p&gt;to protect turbine airfoils from being damaged by hot flue gases. Film injection holes are&lt;/p&gt; &lt;p&gt;placed in the body of the airfoil to allow coolant to pass from the internal cavity to the&lt;/p&gt; &lt;p&gt;external surface. The ejection of coolant gas results in a layer or “film” of coolant gas&lt;/p&gt; &lt;p&gt;flowing along the external surface of the airfoil.&lt;/p&gt; &lt;p&gt;In this study, a new cooling scheme, mist/air film cooling is proposed and&lt;/p&gt; &lt;p&gt;investigated through experiments. Small amount of tiny water droplets with an average&lt;/p&gt; &lt;p&gt;diameter about 7 μm (mist) is injected into the cooling air to enhance the cooling&lt;/p&gt; &lt;p&gt;performance. A wind tunnel system and test facilities were build. A Phase Doppler&lt;/p&gt; &lt;p&gt;Particle Analyzer (PDPA) system is employed to measure droplet size, velocity and&lt;/p&gt; &lt;p&gt;turbulence. Infrared camera and thermocouples are both used for temperature&lt;/p&gt; &lt;p&gt;measurements.&lt;/p&gt; &lt;p&gt;Mist film cooling performance is evaluated and compared against air-only film&lt;/p&gt; &lt;p&gt;cooling in terms of adiabatic film cooling effectiveness and film coverage. Experimental&lt;/p&gt; &lt;p&gt;results show that for blowing ratio M=0.6, net enhancement in adiabatic cooling&lt;/p&gt; &lt;p&gt;effectiveness can reach 190% locally and 128% overall along the centerline. The general&lt;/p&gt; &lt;p&gt;pattern of adiabatic cooling effectiveness distribution of the mist case is similar to that of&lt;/p&gt; &lt;p&gt;the air-only case with the peak at about the same location.&lt;/p&gt; &lt;p&gt;The concept of Film Decay Length (FDL) is proposed to quantitatively evaluate&lt;/p&gt; &lt;p&gt;how well the coolant film covers the blade surface. Application of mist in the M=0.6&lt;/p&gt; &lt;p&gt;condition is apparently superior to the M=1.0 and 1.4 cases due to the higher overall&lt;/p&gt; &lt;p&gt;cooling enhancement, the much longer FDL, and wider and longer film cooling coverage&lt;/p&gt; &lt;p&gt;area.&lt;/p&gt; &lt;p&gt;Based on droplet measurements through PDPA, a profile describing how the airmist&lt;/p&gt; &lt;p&gt;coolant jet flow spreads and eventually blends into the hot main flow is proposed. A&lt;/p&gt; &lt;p&gt;sketch based on the proposed profile is provided. This profile is found to be well&lt;/p&gt; &lt;p&gt;supported by the measurement results of Turbulent Reynolds Stress. The location where&lt;/p&gt; &lt;p&gt;a higher magnitude of Turbulent Reynolds Stress exists, which indicates higher strength&lt;/p&gt; &lt;p&gt;of turbulent mixing effect, is found to be in the close neighborhood of the edge of the&lt;/p&gt; &lt;p&gt;coolant film envelope. Also the separation between the mist droplets layer and the&lt;/p&gt; &lt;p&gt;coolant air film is identified through the measurements. In other words, large droplets&lt;/p&gt; &lt;p&gt;penetrate through the air coolant film layer and travel further over into the main flow.&lt;/p&gt; &lt;p&gt;Based on the proposed air-mist film profile, the heat transfer results are reexamined.&lt;/p&gt; &lt;p&gt;It is found that the location of optimum cooling effect is coincident with the&lt;/p&gt; &lt;p&gt;starting point where the air-mist coolant starts to bend towards the surface. Thus the data&lt;/p&gt; &lt;p&gt;suggests that the “bending back” film pattern is critical in keeping the mist droplets close&lt;/p&gt; &lt;p&gt;to the surface which improves the cooling effectiveness for mist cooling.&lt;/p&gt;","abstract_has_math":false,"creators":["zhao, lei"],"institution":null,"degree_name":"Ph.D.","degree_level":"Dissertation-Restricted","degree_discipline":"Mechanical Engineering","degree_department":null,"school":null,"contributors":["Dr. Ting Wang"],"advisors":[],"committee_chairs":[],"committee_members":[],"year":2012,"date_issued":"2012-05-18T07:00:00Z","date_published":"2012-05-18T07:00:00Z","updated_at":"2026-07-24T05:29:36Z","subjects":["gas turbine","turbine airfoil","heat transfer","film cooling","experimental study","mist cooling","Engineering","Heat Transfer, Combustion","Mechanical Engineering"],"languages":[],"rights":[],"rights_urls":[],"identifier_entries":[]},"links":{"outbound_url":"https://scholarworks.uno.edu/td/1499","outbound_label":"Repository record","outbound_source":"dc:identifier"},"metadata_groups":[{"id":"people","label":"People","entries":[{"key":"dc:contributor","label":"Contributor","values":["Dr. Ting Wang"]},{"key":"dc:creator","label":"Author","values":["zhao, lei"]}]},{"id":"academic_context","label":"Academic Context","entries":[{"key":"thesis:degree_discipline","label":"Discipline","values":["Mechanical Engineering"]},{"key":"thesis:degree_level","label":"Degree Level","values":["Dissertation-Restricted"]},{"key":"thesis:degree_name","label":"Degree Name","values":["Ph.D."]}]},{"id":"subjects_keywords","label":"Subjects and Keywords","entries":[{"key":"dc:subject","label":"Dc Subject","values":["gas turbine","turbine airfoil","heat transfer","film cooling","experimental study","mist cooling","Engineering","Heat Transfer, Combustion","Mechanical Engineering"]}]},{"id":"identifiers","label":"Identifiers","entries":[{"key":"dc:identifier","label":"Identifier","values":["https://scholarworks.uno.edu/td/1499"]}]},{"id":"additional","label":"Additional Metadata","entries":[{"key":"dc:description.abstract","label":"Abstract","values":["<p>Film cooling is a cooling technique widely used in high-performance gas turbines</p> <p>to protect turbine airfoils from being damaged by hot flue gases. Film injection holes are</p> <p>placed in the body of the airfoil to allow coolant to pass from the internal cavity to the</p> <p>external surface. The ejection of coolant gas results in a layer or “film” of coolant gas</p> <p>flowing along the external surface of the airfoil.</p> <p>In this study, a new cooling scheme, mist/air film cooling is proposed and</p> <p>investigated through experiments. Small amount of tiny water droplets with an average</p> <p>diameter about 7 μm (mist) is injected into the cooling air to enhance the cooling</p> <p>performance. A wind tunnel system and test facilities were build. A Phase Doppler</p> <p>Particle Analyzer (PDPA) system is employed to measure droplet size, velocity and</p> <p>turbulence. Infrared camera and thermocouples are both used for temperature</p> <p>measurements.</p> <p>Mist film cooling performance is evaluated and compared against air-only film</p> <p>cooling in terms of adiabatic film cooling effectiveness and film coverage. Experimental</p> <p>results show that for blowing ratio M=0.6, net enhancement in adiabatic cooling</p> <p>effectiveness can reach 190% locally and 128% overall along the centerline. The general</p> <p>pattern of adiabatic cooling effectiveness distribution of the mist case is similar to that of</p> <p>the air-only case with the peak at about the same location.</p> <p>The concept of Film Decay Length (FDL) is proposed to quantitatively evaluate</p> <p>how well the coolant film covers the blade surface. Application of mist in the M=0.6</p> <p>condition is apparently superior to the M=1.0 and 1.4 cases due to the higher overall</p> <p>cooling enhancement, the much longer FDL, and wider and longer film cooling coverage</p> <p>area.</p> <p>Based on droplet measurements through PDPA, a profile describing how the airmist</p> <p>coolant jet flow spreads and eventually blends into the hot main flow is proposed. A</p> <p>sketch based on the proposed profile is provided. This profile is found to be well</p> <p>supported by the measurement results of Turbulent Reynolds Stress. The location where</p> <p>a higher magnitude of Turbulent Reynolds Stress exists, which indicates higher strength</p> <p>of turbulent mixing effect, is found to be in the close neighborhood of the edge of the</p> <p>coolant film envelope. Also the separation between the mist droplets layer and the</p> <p>coolant air film is identified through the measurements. In other words, large droplets</p> <p>penetrate through the air coolant film layer and travel further over into the main flow.</p> <p>Based on the proposed air-mist film profile, the heat transfer results are reexamined.</p> <p>It is found that the location of optimum cooling effect is coincident with the</p> <p>starting point where the air-mist coolant starts to bend towards the surface. Thus the data</p> <p>suggests that the “bending back” film pattern is critical in keeping the mist droplets close</p> <p>to the surface which improves the cooling effectiveness for mist cooling.</p>"]},{"key":"dc:title","label":"Title","values":["An Investigation of Mist/Air Film Cooling with Application to Gas Turbine Airfoils"]}]}],"canonical_facts":{"dc:contributor":["Dr. Ting Wang"],"dc:creator":["zhao, lei"],"dc:description.abstract":["<p>Film cooling is a cooling technique widely used in high-performance gas turbines</p> <p>to protect turbine airfoils from being damaged by hot flue gases. Film injection holes are</p> <p>placed in the body of the airfoil to allow coolant to pass from the internal cavity to the</p> <p>external surface. The ejection of coolant gas results in a layer or “film” of coolant gas</p> <p>flowing along the external surface of the airfoil.</p> <p>In this study, a new cooling scheme, mist/air film cooling is proposed and</p> <p>investigated through experiments. Small amount of tiny water droplets with an average</p> <p>diameter about 7 μm (mist) is injected into the cooling air to enhance the cooling</p> <p>performance. A wind tunnel system and test facilities were build. A Phase Doppler</p> <p>Particle Analyzer (PDPA) system is employed to measure droplet size, velocity and</p> <p>turbulence. Infrared camera and thermocouples are both used for temperature</p> <p>measurements.</p> <p>Mist film cooling performance is evaluated and compared against air-only film</p> <p>cooling in terms of adiabatic film cooling effectiveness and film coverage. Experimental</p> <p>results show that for blowing ratio M=0.6, net enhancement in adiabatic cooling</p> <p>effectiveness can reach 190% locally and 128% overall along the centerline. The general</p> <p>pattern of adiabatic cooling effectiveness distribution of the mist case is similar to that of</p> <p>the air-only case with the peak at about the same location.</p> <p>The concept of Film Decay Length (FDL) is proposed to quantitatively evaluate</p> <p>how well the coolant film covers the blade surface. Application of mist in the M=0.6</p> <p>condition is apparently superior to the M=1.0 and 1.4 cases due to the higher overall</p> <p>cooling enhancement, the much longer FDL, and wider and longer film cooling coverage</p> <p>area.</p> <p>Based on droplet measurements through PDPA, a profile describing how the airmist</p> <p>coolant jet flow spreads and eventually blends into the hot main flow is proposed. A</p> <p>sketch based on the proposed profile is provided. This profile is found to be well</p> <p>supported by the measurement results of Turbulent Reynolds Stress. The location where</p> <p>a higher magnitude of Turbulent Reynolds Stress exists, which indicates higher strength</p> <p>of turbulent mixing effect, is found to be in the close neighborhood of the edge of the</p> <p>coolant film envelope. Also the separation between the mist droplets layer and the</p> <p>coolant air film is identified through the measurements. In other words, large droplets</p> <p>penetrate through the air coolant film layer and travel further over into the main flow.</p> <p>Based on the proposed air-mist film profile, the heat transfer results are reexamined.</p> <p>It is found that the location of optimum cooling effect is coincident with the</p> <p>starting point where the air-mist coolant starts to bend towards the surface. Thus the data</p> <p>suggests that the “bending back” film pattern is critical in keeping the mist droplets close</p> <p>to the surface which improves the cooling effectiveness for mist cooling.</p>"],"dc:identifier":["https://scholarworks.uno.edu/td/1499"],"dc:subject":["gas turbine","turbine airfoil","heat transfer","film cooling","experimental study","mist cooling","Engineering","Heat Transfer, Combustion","Mechanical Engineering"],"dc:title":["An Investigation of Mist/Air Film Cooling with Application to Gas Turbine Airfoils"],"thesis:degree_discipline":["Mechanical Engineering"],"thesis:degree_level":["Dissertation-Restricted"],"thesis:degree_name":["Ph.D."]},"updated_at":"2026-07-24T05:29:36Z"}