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Sourabh S Diwan, Katepalli R Sreenivasan<\/span><\/strong>, 2025<\/span>, “History of Indic sciences and philosophy as viewed by Professor Narasimha<\/a><\/span>” , S\u0101dhan\u0101 50 (1), 28<\/strong><\/p>\n <\/p>\n <\/p>\n [\/et_pb_blurb][et_pb_blurb use_icon=”on” font_icon=”%%59%%” icon_color=”#bda392″ icon_placement=”left” image_icon_width=”27px” content_max_width=”900px” image_icon_width_phone=”101px” image_icon_width_last_edited=”on|phone” _builder_version=”4.18.0″ _module_preset=”default” header_font=”Nunito|700|||||||” header_font_size=”16px” body_font=”Nunito||||||||” body_font_size=”17px” body_link_text_color=”#727272″ vertical_offset_tablet=”0″ horizontal_offset_tablet=”0″ z_index_tablet=”0″ header_text_shadow_horizontal_length_tablet=”0px” header_text_shadow_vertical_length_tablet=”0px” header_text_shadow_blur_strength_tablet=”1px” body_text_shadow_horizontal_length_tablet=”0px” body_text_shadow_vertical_length_tablet=”0px” body_text_shadow_blur_strength_tablet=”1px” body_link_text_shadow_horizontal_length_tablet=”0px” body_link_text_shadow_vertical_length_tablet=”0px” body_link_text_shadow_blur_strength_tablet=”1px” body_ul_text_shadow_horizontal_length_tablet=”0px” body_ul_text_shadow_vertical_length_tablet=”0px” body_ul_text_shadow_blur_strength_tablet=”1px” body_ol_text_shadow_horizontal_length_tablet=”0px” body_ol_text_shadow_vertical_length_tablet=”0px” body_ol_text_shadow_blur_strength_tablet=”1px” body_quote_text_shadow_horizontal_length_tablet=”0px” body_quote_text_shadow_vertical_length_tablet=”0px” body_quote_text_shadow_blur_strength_tablet=”1px” box_shadow_horizontal_tablet=”0px” box_shadow_vertical_tablet=”0px” box_shadow_blur_tablet=”40px” box_shadow_spread_tablet=”0px” box_shadow_horizontal_image_tablet=”0px” box_shadow_vertical_image_tablet=”0px” box_shadow_blur_image_tablet=”40px” box_shadow_spread_image_tablet=”0px” text_shadow_horizontal_length_tablet=”0px” text_shadow_vertical_length_tablet=”0px” text_shadow_blur_strength_tablet=”1px” global_colors_info=”{}” background_pattern_color=”rgba(0,0,0,0.2)” background_mask_color=”#ffffff” text_shadow_horizontal_length=”text_shadow_style,%91object Object%93″ text_shadow_vertical_length=”text_shadow_style,%91object Object%93″ text_shadow_blur_strength=”text_shadow_style,%91object Object%93″ header_text_shadow_horizontal_length=”header_text_shadow_style,%91object Object%93″ header_text_shadow_vertical_length=”header_text_shadow_style,%91object Object%93″ header_text_shadow_blur_strength=”header_text_shadow_style,%91object Object%93″ body_text_shadow_horizontal_length=”body_text_shadow_style,%91object Object%93″ body_text_shadow_vertical_length=”body_text_shadow_style,%91object Object%93″ body_text_shadow_blur_strength=”body_text_shadow_style,%91object Object%93″ body_link_text_shadow_horizontal_length=”body_link_text_shadow_style,%91object Object%93″ body_link_text_shadow_vertical_length=”body_link_text_shadow_style,%91object Object%93″ body_link_text_shadow_blur_strength=”body_link_text_shadow_style,%91object Object%93″ body_ul_text_shadow_horizontal_length=”body_ul_text_shadow_style,%91object Object%93″ body_ul_text_shadow_vertical_length=”body_ul_text_shadow_style,%91object Object%93″ body_ul_text_shadow_blur_strength=”body_ul_text_shadow_style,%91object Object%93″ body_ol_text_shadow_horizontal_length=”body_ol_text_shadow_style,%91object Object%93″ body_ol_text_shadow_vertical_length=”body_ol_text_shadow_style,%91object Object%93″ body_ol_text_shadow_blur_strength=”body_ol_text_shadow_style,%91object Object%93″ body_quote_text_shadow_horizontal_length=”body_quote_text_shadow_style,%91object Object%93″ body_quote_text_shadow_vertical_length=”body_quote_text_shadow_style,%91object Object%93″ body_quote_text_shadow_blur_strength=”body_quote_text_shadow_style,%91object Object%93″]<\/p>\n A Anand, S Diwan, N Swaminathan<\/strong>, 2024<\/span>, “A comparative study of bandpass-filter-based multi-scale methods for turbulence energy cascade<\/a><\/span>” , Journal of Turbulence 25 (12), 451-460<\/strong><\/p>\n <\/p>\n <\/p>\n [\/et_pb_blurb][et_pb_blurb use_icon=”on” font_icon=”%%59%%” icon_color=”#bda392″ icon_placement=”left” image_icon_width=”27px” content_max_width=”900px” image_icon_width_last_edited=”on|phone” _builder_version=”4.18.0″ _module_preset=”default” header_font=”Nunito|700|||||||” header_font_size=”16px” body_font=”Nunito||||||||” body_font_size=”17px” body_link_text_color=”#727272″ vertical_offset_tablet=”0″ horizontal_offset_tablet=”0″ z_index_tablet=”0″ header_text_shadow_horizontal_length_tablet=”0px” header_text_shadow_vertical_length_tablet=”0px” header_text_shadow_blur_strength_tablet=”1px” body_text_shadow_horizontal_length_tablet=”0px” body_text_shadow_vertical_length_tablet=”0px” body_text_shadow_blur_strength_tablet=”1px” body_link_text_shadow_horizontal_length_tablet=”0px” body_link_text_shadow_vertical_length_tablet=”0px” body_link_text_shadow_blur_strength_tablet=”1px” body_ul_text_shadow_horizontal_length_tablet=”0px” body_ul_text_shadow_vertical_length_tablet=”0px” body_ul_text_shadow_blur_strength_tablet=”1px” body_ol_text_shadow_horizontal_length_tablet=”0px” body_ol_text_shadow_vertical_length_tablet=”0px” body_ol_text_shadow_blur_strength_tablet=”1px” body_quote_text_shadow_horizontal_length_tablet=”0px” body_quote_text_shadow_vertical_length_tablet=”0px” body_quote_text_shadow_blur_strength_tablet=”1px” box_shadow_horizontal_tablet=”0px” box_shadow_vertical_tablet=”0px” box_shadow_blur_tablet=”40px” box_shadow_spread_tablet=”0px” box_shadow_horizontal_image_tablet=”0px” box_shadow_vertical_image_tablet=”0px” box_shadow_blur_image_tablet=”40px” box_shadow_spread_image_tablet=”0px” text_shadow_horizontal_length_tablet=”0px” text_shadow_vertical_length_tablet=”0px” text_shadow_blur_strength_tablet=”1px” global_colors_info=”{}”]<\/p>\n S. De, Aditya Anand, and Sourabh S. Diwan, <\/strong>2023,<\/strong> “A wavelet-based detector function for characterizing intermittent velocity signals”,\u00a0 Exp Fluids<\/i><\/strong> 64<\/b>, 180<\/strong><\/p>\n [\/et_pb_blurb][et_pb_blurb use_icon=”on” font_icon=”%%59%%” icon_color=”#bda392″ icon_placement=”left” image_icon_width=”27px” content_max_width=”900px” image_icon_width_last_edited=”on|phone” _builder_version=”4.18.0″ _module_preset=”default” header_font=”Nunito|700|||||||” header_font_size=”16px” body_font=”Nunito||||||||” body_font_size=”17px” body_link_text_color=”#727272″ vertical_offset_tablet=”0″ horizontal_offset_tablet=”0″ z_index_tablet=”0″ header_text_shadow_horizontal_length_tablet=”0px” header_text_shadow_vertical_length_tablet=”0px” header_text_shadow_blur_strength_tablet=”1px” body_text_shadow_horizontal_length_tablet=”0px” body_text_shadow_vertical_length_tablet=”0px” body_text_shadow_blur_strength_tablet=”1px” body_link_text_shadow_horizontal_length_tablet=”0px” body_link_text_shadow_vertical_length_tablet=”0px” body_link_text_shadow_blur_strength_tablet=”1px” body_ul_text_shadow_horizontal_length_tablet=”0px” body_ul_text_shadow_vertical_length_tablet=”0px” body_ul_text_shadow_blur_strength_tablet=”1px” body_ol_text_shadow_horizontal_length_tablet=”0px” body_ol_text_shadow_vertical_length_tablet=”0px” body_ol_text_shadow_blur_strength_tablet=”1px” body_quote_text_shadow_horizontal_length_tablet=”0px” body_quote_text_shadow_vertical_length_tablet=”0px” body_quote_text_shadow_blur_strength_tablet=”1px” box_shadow_horizontal_tablet=”0px” box_shadow_vertical_tablet=”0px” box_shadow_blur_tablet=”40px” box_shadow_spread_tablet=”0px” box_shadow_horizontal_image_tablet=”0px” box_shadow_vertical_image_tablet=”0px” box_shadow_blur_image_tablet=”40px” box_shadow_spread_image_tablet=”0px” text_shadow_horizontal_length_tablet=”0px” text_shadow_vertical_length_tablet=”0px” text_shadow_blur_strength_tablet=”1px” global_colors_info=”{}”]<\/p>\n <\/strong>S. De, Aditya Anand, and Sourabh S. Diwan, <\/strong>2023,<\/strong> “A wavelet-based detector function for characterizing intermittent velocity signals”,\u00a0 Exp Fluids<\/i><\/strong> 64<\/b>, 180<\/strong><\/p>\n [\/et_pb_blurb][et_pb_blurb use_icon=”on” font_icon=”%%59%%” icon_color=”#bda392″ icon_placement=”left” image_icon_width=”27px” content_max_width=”900px” image_icon_width_last_edited=”on|phone” _builder_version=”4.18.0″ _module_preset=”default” header_font=”Nunito|700|||||||” header_font_size=”16px” body_font=”Nunito||||||||” body_font_size=”17px” body_link_text_color=”#727272″ vertical_offset_tablet=”0″ horizontal_offset_tablet=”0″ z_index_tablet=”0″ header_text_shadow_horizontal_length_tablet=”0px” header_text_shadow_vertical_length_tablet=”0px” header_text_shadow_blur_strength_tablet=”1px” body_text_shadow_horizontal_length_tablet=”0px” body_text_shadow_vertical_length_tablet=”0px” body_text_shadow_blur_strength_tablet=”1px” body_link_text_shadow_horizontal_length_tablet=”0px” body_link_text_shadow_vertical_length_tablet=”0px” body_link_text_shadow_blur_strength_tablet=”1px” body_ul_text_shadow_horizontal_length_tablet=”0px” body_ul_text_shadow_vertical_length_tablet=”0px” body_ul_text_shadow_blur_strength_tablet=”1px” body_ol_text_shadow_horizontal_length_tablet=”0px” body_ol_text_shadow_vertical_length_tablet=”0px” body_ol_text_shadow_blur_strength_tablet=”1px” body_quote_text_shadow_horizontal_length_tablet=”0px” body_quote_text_shadow_vertical_length_tablet=”0px” body_quote_text_shadow_blur_strength_tablet=”1px” box_shadow_horizontal_tablet=”0px” box_shadow_vertical_tablet=”0px” box_shadow_blur_tablet=”40px” box_shadow_spread_tablet=”0px” box_shadow_horizontal_image_tablet=”0px” box_shadow_vertical_image_tablet=”0px” box_shadow_blur_image_tablet=”40px” box_shadow_spread_image_tablet=”0px” text_shadow_horizontal_length_tablet=”0px” text_shadow_vertical_length_tablet=”0px” text_shadow_blur_strength_tablet=”1px” global_colors_info=”{}”]<\/p>\n Rohit Singhal, S. Ravichandran, and Sourabh S. Diwan<\/strong>, 2022 \u201cDirect Numerical Simulation of a Moist Cough Flow using Eulerian Approximation for Liquid Droplets\u201d, Int. J. Comput. Fluid Dyn.,<\/em><\/strong> 35(9)<\/strong>, 778-797 (Invited article<\/em><\/strong> for a special issue on<\/em> \u201cCFD and COVID 19\u201d<\/em>)<\/p>\n [\/et_pb_blurb][et_pb_blurb use_icon=”on” font_icon=”%%59%%” icon_color=”#bda392″ icon_placement=”left” image_icon_width=”27px” content_max_width=”900px” image_icon_width_last_edited=”on|phone” _builder_version=”4.18.0″ _module_preset=”default” header_font=”Nunito|700|||||||” header_font_size=”16px” body_font=”Nunito||||||||” body_font_size=”17px” body_link_text_color=”#727272″ vertical_offset_tablet=”0″ horizontal_offset_tablet=”0″ z_index_tablet=”0″ header_text_shadow_horizontal_length_tablet=”0px” header_text_shadow_vertical_length_tablet=”0px” header_text_shadow_blur_strength_tablet=”1px” body_text_shadow_horizontal_length_tablet=”0px” body_text_shadow_vertical_length_tablet=”0px” body_text_shadow_blur_strength_tablet=”1px” body_link_text_shadow_horizontal_length_tablet=”0px” body_link_text_shadow_vertical_length_tablet=”0px” body_link_text_shadow_blur_strength_tablet=”1px” body_ul_text_shadow_horizontal_length_tablet=”0px” body_ul_text_shadow_vertical_length_tablet=”0px” body_ul_text_shadow_blur_strength_tablet=”1px” body_ol_text_shadow_horizontal_length_tablet=”0px” body_ol_text_shadow_vertical_length_tablet=”0px” body_ol_text_shadow_blur_strength_tablet=”1px” body_quote_text_shadow_horizontal_length_tablet=”0px” body_quote_text_shadow_vertical_length_tablet=”0px” body_quote_text_shadow_blur_strength_tablet=”1px” box_shadow_horizontal_tablet=”0px” box_shadow_vertical_tablet=”0px” box_shadow_blur_tablet=”40px” box_shadow_spread_tablet=”0px” box_shadow_horizontal_image_tablet=”0px” box_shadow_vertical_image_tablet=”0px” box_shadow_blur_image_tablet=”40px” box_shadow_spread_image_tablet=”0px” text_shadow_horizontal_length_tablet=”0px” text_shadow_vertical_length_tablet=”0px” text_shadow_blur_strength_tablet=”1px” global_colors_info=”{}”]<\/p>\n A.B. Aadhishwaran and Sourabh S. Diwan<\/strong>, 2021 \u201cPredominance of pressure transport in spatial energy budget for a mixing layer approaching absolute instability\u201d, Phys. Rev. Fluids<\/em><\/strong>, 6<\/strong>, L091901<\/p>\n [\/et_pb_blurb][et_pb_blurb use_icon=”on” font_icon=”%%59%%” icon_color=”#bda392″ icon_placement=”left” image_icon_width=”27px” content_max_width=”900px” image_icon_width_last_edited=”on|phone” _builder_version=”4.18.0″ _module_preset=”default” header_font=”Nunito|700|||||||” header_font_size=”16px” body_font=”Nunito||||||||” body_font_size=”17px” body_link_text_color=”#727272″ vertical_offset_tablet=”0″ horizontal_offset_tablet=”0″ z_index_tablet=”0″ header_text_shadow_horizontal_length_tablet=”0px” header_text_shadow_vertical_length_tablet=”0px” header_text_shadow_blur_strength_tablet=”1px” body_text_shadow_horizontal_length_tablet=”0px” body_text_shadow_vertical_length_tablet=”0px” body_text_shadow_blur_strength_tablet=”1px” body_link_text_shadow_horizontal_length_tablet=”0px” body_link_text_shadow_vertical_length_tablet=”0px” body_link_text_shadow_blur_strength_tablet=”1px” body_ul_text_shadow_horizontal_length_tablet=”0px” body_ul_text_shadow_vertical_length_tablet=”0px” body_ul_text_shadow_blur_strength_tablet=”1px” body_ol_text_shadow_horizontal_length_tablet=”0px” body_ol_text_shadow_vertical_length_tablet=”0px” body_ol_text_shadow_blur_strength_tablet=”1px” body_quote_text_shadow_horizontal_length_tablet=”0px” body_quote_text_shadow_vertical_length_tablet=”0px” body_quote_text_shadow_blur_strength_tablet=”1px” box_shadow_horizontal_tablet=”0px” box_shadow_vertical_tablet=”0px” box_shadow_blur_tablet=”40px” box_shadow_spread_tablet=”0px” box_shadow_horizontal_image_tablet=”0px” box_shadow_vertical_image_tablet=”0px” box_shadow_blur_image_tablet=”40px” box_shadow_spread_image_tablet=”0px” text_shadow_horizontal_length_tablet=”0px” text_shadow_vertical_length_tablet=”0px” text_shadow_blur_strength_tablet=”1px” global_colors_info=”{}”]<\/p>\n A. Samson, Karthik Naicker and Sourabh S. Diwan<\/strong>, 2021 \u201cInstability mechanisms and intermittency distribution in adverse pressure gradient attached and separated boundary layers\u201d, Phys. Fluids<\/em><\/strong>, 33<\/strong>, 094106 (Invited article<\/em><\/strong>: Special Topic on Tribute to Frank M. White on his 88th anniversary<\/em>)<\/p>\n [\/et_pb_blurb][et_pb_blurb use_icon=”on” font_icon=”%%59%%” icon_color=”#bda392″ icon_placement=”left” image_icon_width=”27px” content_max_width=”900px” image_icon_width_last_edited=”on|phone” _builder_version=”4.18.0″ _module_preset=”default” header_font=”Nunito|700|||||||” header_font_size=”16px” body_font=”Nunito||||||||” body_font_size=”17px” body_link_text_color=”#727272″ vertical_offset_tablet=”0″ horizontal_offset_tablet=”0″ z_index_tablet=”0″ header_text_shadow_horizontal_length_tablet=”0px” header_text_shadow_vertical_length_tablet=”0px” header_text_shadow_blur_strength_tablet=”1px” body_text_shadow_horizontal_length_tablet=”0px” body_text_shadow_vertical_length_tablet=”0px” body_text_shadow_blur_strength_tablet=”1px” body_link_text_shadow_horizontal_length_tablet=”0px” body_link_text_shadow_vertical_length_tablet=”0px” body_link_text_shadow_blur_strength_tablet=”1px” body_ul_text_shadow_horizontal_length_tablet=”0px” body_ul_text_shadow_vertical_length_tablet=”0px” body_ul_text_shadow_blur_strength_tablet=”1px” body_ol_text_shadow_horizontal_length_tablet=”0px” body_ol_text_shadow_vertical_length_tablet=”0px” body_ol_text_shadow_blur_strength_tablet=”1px” body_quote_text_shadow_horizontal_length_tablet=”0px” body_quote_text_shadow_vertical_length_tablet=”0px” body_quote_text_shadow_blur_strength_tablet=”1px” box_shadow_horizontal_tablet=”0px” box_shadow_vertical_tablet=”0px” box_shadow_blur_tablet=”40px” box_shadow_spread_tablet=”0px” box_shadow_horizontal_image_tablet=”0px” box_shadow_vertical_image_tablet=”0px” box_shadow_blur_image_tablet=”40px” box_shadow_spread_image_tablet=”0px” text_shadow_horizontal_length_tablet=”0px” text_shadow_vertical_length_tablet=”0px” text_shadow_blur_strength_tablet=”1px” global_colors_info=”{}”]<\/p>\n Srinivas Kirthy K. and Sourabh S. Diwan<\/strong>, 2021 \u201cEnergy budget analysis and neutral curve characteristics for the linear instability of Couette\u2013Poiseuille flow\u201d, Phys. Fluids<\/em><\/strong>, 33<\/strong>, 034102.<\/p>\n [\/et_pb_blurb][et_pb_blurb use_icon=”on” font_icon=”%%59%%” icon_color=”#bda392″ icon_placement=”left” image_icon_width=”27px” content_max_width=”900px” image_icon_width_last_edited=”on|phone” _builder_version=”4.18.0″ _module_preset=”default” header_font=”Nunito|700|||||||” header_font_size=”16px” body_font=”Nunito||||||||” body_font_size=”17px” body_link_text_color=”#727272″ vertical_offset_tablet=”0″ horizontal_offset_tablet=”0″ z_index_tablet=”0″ header_text_shadow_horizontal_length_tablet=”0px” header_text_shadow_vertical_length_tablet=”0px” header_text_shadow_blur_strength_tablet=”1px” body_text_shadow_horizontal_length_tablet=”0px” body_text_shadow_vertical_length_tablet=”0px” body_text_shadow_blur_strength_tablet=”1px” body_link_text_shadow_horizontal_length_tablet=”0px” body_link_text_shadow_vertical_length_tablet=”0px” body_link_text_shadow_blur_strength_tablet=”1px” body_ul_text_shadow_horizontal_length_tablet=”0px” body_ul_text_shadow_vertical_length_tablet=”0px” body_ul_text_shadow_blur_strength_tablet=”1px” body_ol_text_shadow_horizontal_length_tablet=”0px” body_ol_text_shadow_vertical_length_tablet=”0px” body_ol_text_shadow_blur_strength_tablet=”1px” body_quote_text_shadow_horizontal_length_tablet=”0px” body_quote_text_shadow_vertical_length_tablet=”0px” body_quote_text_shadow_blur_strength_tablet=”1px” box_shadow_horizontal_tablet=”0px” box_shadow_vertical_tablet=”0px” box_shadow_blur_tablet=”40px” box_shadow_spread_tablet=”0px” box_shadow_horizontal_image_tablet=”0px” box_shadow_vertical_image_tablet=”0px” box_shadow_blur_image_tablet=”40px” box_shadow_spread_image_tablet=”0px” text_shadow_horizontal_length_tablet=”0px” text_shadow_vertical_length_tablet=”0px” text_shadow_blur_strength_tablet=”1px” global_colors_info=”{}”]<\/p>\n Sourabh S. Diwan and Jonathan F. Morrison<\/strong>, 2021 \u201cIntermediate Scaling and Logarithmic Invariance in Turbulent Pipe Flow\u201d, J. Fluid Mech.<\/em>,<\/strong> 913<\/strong>, R1.<\/p>\n [\/et_pb_blurb][et_pb_blurb use_icon=”on” font_icon=”%%59%%” icon_color=”#bda392″ icon_placement=”left” image_icon_width=”27px” content_max_width=”900px” image_icon_width_last_edited=”on|phone” _builder_version=”4.18.0″ _module_preset=”default” header_font=”Nunito|700|||||||” header_font_size=”16px” body_font=”Nunito||||||||” body_font_size=”17px” body_link_text_color=”#727272″ vertical_offset_tablet=”0″ horizontal_offset_tablet=”0″ z_index_tablet=”0″ header_text_shadow_horizontal_length_tablet=”0px” header_text_shadow_vertical_length_tablet=”0px” header_text_shadow_blur_strength_tablet=”1px” body_text_shadow_horizontal_length_tablet=”0px” body_text_shadow_vertical_length_tablet=”0px” body_text_shadow_blur_strength_tablet=”1px” body_link_text_shadow_horizontal_length_tablet=”0px” body_link_text_shadow_vertical_length_tablet=”0px” body_link_text_shadow_blur_strength_tablet=”1px” body_ul_text_shadow_horizontal_length_tablet=”0px” body_ul_text_shadow_vertical_length_tablet=”0px” body_ul_text_shadow_blur_strength_tablet=”1px” body_ol_text_shadow_horizontal_length_tablet=”0px” body_ol_text_shadow_vertical_length_tablet=”0px” body_ol_text_shadow_blur_strength_tablet=”1px” body_quote_text_shadow_horizontal_length_tablet=”0px” body_quote_text_shadow_vertical_length_tablet=”0px” body_quote_text_shadow_blur_strength_tablet=”1px” box_shadow_horizontal_tablet=”0px” box_shadow_vertical_tablet=”0px” box_shadow_blur_tablet=”40px” box_shadow_spread_tablet=”0px” box_shadow_horizontal_image_tablet=”0px” box_shadow_vertical_image_tablet=”0px” box_shadow_blur_image_tablet=”40px” box_shadow_spread_image_tablet=”0px” text_shadow_horizontal_length_tablet=”0px” text_shadow_vertical_length_tablet=”0px” text_shadow_blur_strength_tablet=”1px” global_colors_info=”{}”]<\/p>\n Sourabh S. Diwan, S. Ravichandran, Rama Govindarajan, Roddam Narasimha<\/strong>, 2020 \u201cUnderstanding Transmission Dynamics of COVID\u201119\u2011Type Infections by Direct Numerical Simulations of Cough\/Sneeze Flows\u201d, Trans. Indian Natl. Acad. Eng.<\/em><\/strong>, June-3<\/strong>, 1-7.<\/p>\n [\/et_pb_blurb][et_pb_blurb use_icon=”on” font_icon=”%%59%%” icon_color=”#bda392″ icon_placement=”left” image_icon_width=”27px” content_max_width=”900px” image_icon_width_last_edited=”on|phone” _builder_version=”4.18.0″ _module_preset=”default” header_font=”Nunito|700|||||||” header_font_size=”16px” body_font=”Nunito||||||||” body_font_size=”17px” body_link_text_color=”#727272″ vertical_offset_tablet=”0″ horizontal_offset_tablet=”0″ z_index_tablet=”0″ header_text_shadow_horizontal_length_tablet=”0px” header_text_shadow_vertical_length_tablet=”0px” header_text_shadow_blur_strength_tablet=”1px” body_text_shadow_horizontal_length_tablet=”0px” body_text_shadow_vertical_length_tablet=”0px” body_text_shadow_blur_strength_tablet=”1px” body_link_text_shadow_horizontal_length_tablet=”0px” body_link_text_shadow_vertical_length_tablet=”0px” body_link_text_shadow_blur_strength_tablet=”1px” body_ul_text_shadow_horizontal_length_tablet=”0px” body_ul_text_shadow_vertical_length_tablet=”0px” body_ul_text_shadow_blur_strength_tablet=”1px” body_ol_text_shadow_horizontal_length_tablet=”0px” body_ol_text_shadow_vertical_length_tablet=”0px” body_ol_text_shadow_blur_strength_tablet=”1px” body_quote_text_shadow_horizontal_length_tablet=”0px” body_quote_text_shadow_vertical_length_tablet=”0px” body_quote_text_shadow_blur_strength_tablet=”1px” box_shadow_horizontal_tablet=”0px” box_shadow_vertical_tablet=”0px” box_shadow_blur_tablet=”40px” box_shadow_spread_tablet=”0px” box_shadow_horizontal_image_tablet=”0px” box_shadow_vertical_image_tablet=”0px” box_shadow_blur_image_tablet=”40px” box_shadow_spread_image_tablet=”0px” text_shadow_horizontal_length_tablet=”0px” text_shadow_vertical_length_tablet=”0px” text_shadow_blur_strength_tablet=”1px” global_colors_info=”{}”]<\/p>\n Aditya Anand and Sourabh S. Diwan, <\/strong>2020 \u201cTime\u2011frequency analysis for two cases of boundary\u2011layer transition induced by random distributed roughness\u201d, Exp. Fluids<\/em><\/strong>, 61<\/strong>:60.<\/p>\n [\/et_pb_blurb][et_pb_blurb use_icon=”on” font_icon=”%%59%%” icon_color=”#bda392″ icon_placement=”left” image_icon_width=”27px” content_max_width=”900px” image_icon_width_last_edited=”on|phone” _builder_version=”4.18.0″ _module_preset=”default” header_font=”Nunito|700|||||||” header_font_size=”16px” body_font=”Nunito||||||||” body_font_size=”17px” body_link_text_color=”#727272″ vertical_offset_tablet=”0″ horizontal_offset_tablet=”0″ z_index_tablet=”0″ header_text_shadow_horizontal_length_tablet=”0px” header_text_shadow_vertical_length_tablet=”0px” header_text_shadow_blur_strength_tablet=”1px” body_text_shadow_horizontal_length_tablet=”0px” body_text_shadow_vertical_length_tablet=”0px” body_text_shadow_blur_strength_tablet=”1px” body_link_text_shadow_horizontal_length_tablet=”0px” body_link_text_shadow_vertical_length_tablet=”0px” body_link_text_shadow_blur_strength_tablet=”1px” body_ul_text_shadow_horizontal_length_tablet=”0px” body_ul_text_shadow_vertical_length_tablet=”0px” body_ul_text_shadow_blur_strength_tablet=”1px” body_ol_text_shadow_horizontal_length_tablet=”0px” body_ol_text_shadow_vertical_length_tablet=”0px” body_ol_text_shadow_blur_strength_tablet=”1px” body_quote_text_shadow_horizontal_length_tablet=”0px” body_quote_text_shadow_vertical_length_tablet=”0px” body_quote_text_shadow_blur_strength_tablet=”1px” box_shadow_horizontal_tablet=”0px” box_shadow_vertical_tablet=”0px” box_shadow_blur_tablet=”40px” box_shadow_spread_tablet=”0px” box_shadow_horizontal_image_tablet=”0px” box_shadow_vertical_image_tablet=”0px” box_shadow_blur_image_tablet=”40px” box_shadow_spread_image_tablet=”0px” text_shadow_horizontal_length_tablet=”0px” text_shadow_vertical_length_tablet=”0px” text_shadow_blur_strength_tablet=”1px” global_colors_info=”{}”]<\/p>\n Sourabh S. Diwan and Jonathan F. Morrison<\/strong>, 2017 \u201cSpectral structure and linear mechanisms in a rapidly-distorted boundary layer\u201d, Int. J. Heat Fluid Flow<\/em><\/strong>, 67<\/strong>, 63-73. (Invited article for the special issue<\/em><\/strong>: Symposium on Experiments and Simulations in Fluid Dynamics Research<\/em>)<\/p>\n [\/et_pb_blurb][et_pb_blurb use_icon=”on” font_icon=”%%59%%” icon_color=”#bda392″ icon_placement=”left” image_icon_width=”27px” content_max_width=”900px” image_icon_width_last_edited=”on|phone” _builder_version=”4.18.0″ _module_preset=”default” header_font=”Nunito|700|||||||” header_font_size=”16px” body_font=”Nunito||||||||” body_font_size=”17px” body_link_text_color=”#727272″ vertical_offset_tablet=”0″ horizontal_offset_tablet=”0″ z_index_tablet=”0″ header_text_shadow_horizontal_length_tablet=”0px” header_text_shadow_vertical_length_tablet=”0px” header_text_shadow_blur_strength_tablet=”1px” body_text_shadow_horizontal_length_tablet=”0px” body_text_shadow_vertical_length_tablet=”0px” body_text_shadow_blur_strength_tablet=”1px” body_link_text_shadow_horizontal_length_tablet=”0px” body_link_text_shadow_vertical_length_tablet=”0px” body_link_text_shadow_blur_strength_tablet=”1px” body_ul_text_shadow_horizontal_length_tablet=”0px” body_ul_text_shadow_vertical_length_tablet=”0px” body_ul_text_shadow_blur_strength_tablet=”1px” body_ol_text_shadow_horizontal_length_tablet=”0px” body_ol_text_shadow_vertical_length_tablet=”0px” body_ol_text_shadow_blur_strength_tablet=”1px” body_quote_text_shadow_horizontal_length_tablet=”0px” body_quote_text_shadow_vertical_length_tablet=”0px” body_quote_text_shadow_blur_strength_tablet=”1px” box_shadow_horizontal_tablet=”0px” box_shadow_vertical_tablet=”0px” box_shadow_blur_tablet=”40px” box_shadow_spread_tablet=”0px” box_shadow_horizontal_image_tablet=”0px” box_shadow_vertical_image_tablet=”0px” box_shadow_blur_image_tablet=”40px” box_shadow_spread_image_tablet=”0px” text_shadow_horizontal_length_tablet=”0px” text_shadow_vertical_length_tablet=”0px” text_shadow_blur_strength_tablet=”1px” global_colors_info=”{}”]<\/p>\n Sourabh S. Diwan<\/strong>, 2015 \u201cNecessary conditions for spatial inviscid instability\u201d, Proc. Roy. Soc. A<\/em><\/strong>, 471<\/strong>, 20140607.<\/p>\n [\/et_pb_blurb][et_pb_blurb use_icon=”on” font_icon=”%%59%%” icon_color=”#bda392″ icon_placement=”left” image_icon_width=”27px” content_max_width=”900px” image_icon_width_last_edited=”on|phone” _builder_version=”4.18.0″ _module_preset=”default” header_font=”Nunito|700|||||||” header_font_size=”16px” body_font=”Nunito||||||||” body_font_size=”17px” body_link_text_color=”#727272″ vertical_offset_tablet=”0″ horizontal_offset_tablet=”0″ z_index_tablet=”0″ header_text_shadow_horizontal_length_tablet=”0px” header_text_shadow_vertical_length_tablet=”0px” header_text_shadow_blur_strength_tablet=”1px” body_text_shadow_horizontal_length_tablet=”0px” body_text_shadow_vertical_length_tablet=”0px” body_text_shadow_blur_strength_tablet=”1px” body_link_text_shadow_horizontal_length_tablet=”0px” body_link_text_shadow_vertical_length_tablet=”0px” body_link_text_shadow_blur_strength_tablet=”1px” body_ul_text_shadow_horizontal_length_tablet=”0px” body_ul_text_shadow_vertical_length_tablet=”0px” body_ul_text_shadow_blur_strength_tablet=”1px” body_ol_text_shadow_horizontal_length_tablet=”0px” body_ol_text_shadow_vertical_length_tablet=”0px” body_ol_text_shadow_blur_strength_tablet=”1px” body_quote_text_shadow_horizontal_length_tablet=”0px” body_quote_text_shadow_vertical_length_tablet=”0px” body_quote_text_shadow_blur_strength_tablet=”1px” box_shadow_horizontal_tablet=”0px” box_shadow_vertical_tablet=”0px” box_shadow_blur_tablet=”40px” box_shadow_spread_tablet=”0px” box_shadow_horizontal_image_tablet=”0px” box_shadow_vertical_image_tablet=”0px” box_shadow_blur_image_tablet=”40px” box_shadow_spread_image_tablet=”0px” text_shadow_horizontal_length_tablet=”0px” text_shadow_vertical_length_tablet=”0px” text_shadow_blur_strength_tablet=”1px” global_colors_info=”{}”]<\/p>\n Sourabh S. Diwan, P. Prasanth, K. R. Sreenivas, S. M. Deshpande and Roddam Narasimha<\/strong>, 2014 \u201cCumulus-type flows in the laboratory and on the computer: simulating cloud form, evolution and large-scale structure\u201d, Bull. Amer. Meteor. Soc<\/em>.,<\/strong> 95(10)<\/strong>, 1541-1548. (Selected under \u2018In Box\u2019 section meant for articles with \u2018Insights and Innovations<\/em>\u2019).<\/p>\n [\/et_pb_blurb][et_pb_blurb use_icon=”on” font_icon=”%%59%%” icon_color=”#bda392″ icon_placement=”left” image_icon_width=”27px” content_max_width=”900px” image_icon_width_last_edited=”on|phone” _builder_version=”4.18.0″ _module_preset=”default” header_font=”Nunito|700|||||||” header_font_size=”16px” body_font=”Nunito||||||||” body_font_size=”17px” body_link_text_color=”#727272″ vertical_offset_tablet=”0″ horizontal_offset_tablet=”0″ z_index_tablet=”0″ header_text_shadow_horizontal_length_tablet=”0px” header_text_shadow_vertical_length_tablet=”0px” header_text_shadow_blur_strength_tablet=”1px” body_text_shadow_horizontal_length_tablet=”0px” body_text_shadow_vertical_length_tablet=”0px” body_text_shadow_blur_strength_tablet=”1px” body_link_text_shadow_horizontal_length_tablet=”0px” body_link_text_shadow_vertical_length_tablet=”0px” body_link_text_shadow_blur_strength_tablet=”1px” body_ul_text_shadow_horizontal_length_tablet=”0px” body_ul_text_shadow_vertical_length_tablet=”0px” body_ul_text_shadow_blur_strength_tablet=”1px” body_ol_text_shadow_horizontal_length_tablet=”0px” body_ol_text_shadow_vertical_length_tablet=”0px” body_ol_text_shadow_blur_strength_tablet=”1px” body_quote_text_shadow_horizontal_length_tablet=”0px” body_quote_text_shadow_vertical_length_tablet=”0px” body_quote_text_shadow_blur_strength_tablet=”1px” box_shadow_horizontal_tablet=”0px” box_shadow_vertical_tablet=”0px” box_shadow_blur_tablet=”40px” box_shadow_spread_tablet=”0px” box_shadow_horizontal_image_tablet=”0px” box_shadow_vertical_image_tablet=”0px” box_shadow_blur_image_tablet=”40px” box_shadow_spread_image_tablet=”0px” text_shadow_horizontal_length_tablet=”0px” text_shadow_vertical_length_tablet=”0px” text_shadow_blur_strength_tablet=”1px” global_colors_info=”{}”]<\/p>\n Sourabh S. Diwan and O. N. Ramesh<\/strong>, 2012 \u201cRelevance of local parallel theory to the linear stability of laminar separation bubbles\u201d J. Fluid Mech.<\/em>,<\/strong> 698<\/strong>, 468-478.<\/p>\n [\/et_pb_blurb][et_pb_blurb use_icon=”on” font_icon=”%%59%%” icon_color=”#bda392″ icon_placement=”left” image_icon_width=”27px” content_max_width=”900px” image_icon_width_last_edited=”on|phone” _builder_version=”4.18.0″ _module_preset=”default” header_font=”Nunito|700|||||||” header_font_size=”16px” body_font=”Nunito||||||||” body_font_size=”17px” body_link_text_color=”#727272″ vertical_offset_tablet=”0″ horizontal_offset_tablet=”0″ z_index_tablet=”0″ header_text_shadow_horizontal_length_tablet=”0px” header_text_shadow_vertical_length_tablet=”0px” header_text_shadow_blur_strength_tablet=”1px” body_text_shadow_horizontal_length_tablet=”0px” body_text_shadow_vertical_length_tablet=”0px” body_text_shadow_blur_strength_tablet=”1px” body_link_text_shadow_horizontal_length_tablet=”0px” body_link_text_shadow_vertical_length_tablet=”0px” body_link_text_shadow_blur_strength_tablet=”1px” body_ul_text_shadow_horizontal_length_tablet=”0px” body_ul_text_shadow_vertical_length_tablet=”0px” body_ul_text_shadow_blur_strength_tablet=”1px” body_ol_text_shadow_horizontal_length_tablet=”0px” body_ol_text_shadow_vertical_length_tablet=”0px” body_ol_text_shadow_blur_strength_tablet=”1px” body_quote_text_shadow_horizontal_length_tablet=”0px” body_quote_text_shadow_vertical_length_tablet=”0px” body_quote_text_shadow_blur_strength_tablet=”1px” box_shadow_horizontal_tablet=”0px” box_shadow_vertical_tablet=”0px” box_shadow_blur_tablet=”40px” box_shadow_spread_tablet=”0px” box_shadow_horizontal_image_tablet=”0px” box_shadow_vertical_image_tablet=”0px” box_shadow_blur_image_tablet=”40px” box_shadow_spread_image_tablet=”0px” text_shadow_horizontal_length_tablet=”0px” text_shadow_vertical_length_tablet=”0px” text_shadow_blur_strength_tablet=”1px” global_colors_info=”{}”]<\/p>\n Sourabh S. Diwan, Roddam Narasimha, G. S. Bhat and K. R. Sreenivas<\/strong>, 2011 \u201cLaboratory studies of anomalous entrainment in cumulus cloud flows\u201d J. Phys.: Conf. Series<\/em><\/strong>, 318<\/strong>, 072014.<\/p>\n [\/et_pb_blurb][et_pb_blurb use_icon=”on” font_icon=”%%59%%” icon_color=”#bda392″ icon_placement=”left” image_icon_width=”27px” content_max_width=”900px” image_icon_width_last_edited=”on|phone” _builder_version=”4.18.0″ _module_preset=”default” header_font=”Nunito|700|||||||” header_font_size=”16px” body_font=”Nunito||||||||” body_font_size=”17px” body_link_text_color=”#727272″ vertical_offset_tablet=”0″ horizontal_offset_tablet=”0″ z_index_tablet=”0″ header_text_shadow_horizontal_length_tablet=”0px” header_text_shadow_vertical_length_tablet=”0px” header_text_shadow_blur_strength_tablet=”1px” body_text_shadow_horizontal_length_tablet=”0px” body_text_shadow_vertical_length_tablet=”0px” body_text_shadow_blur_strength_tablet=”1px” body_link_text_shadow_horizontal_length_tablet=”0px” body_link_text_shadow_vertical_length_tablet=”0px” body_link_text_shadow_blur_strength_tablet=”1px” body_ul_text_shadow_horizontal_length_tablet=”0px” body_ul_text_shadow_vertical_length_tablet=”0px” body_ul_text_shadow_blur_strength_tablet=”1px” body_ol_text_shadow_horizontal_length_tablet=”0px” body_ol_text_shadow_vertical_length_tablet=”0px” body_ol_text_shadow_blur_strength_tablet=”1px” body_quote_text_shadow_horizontal_length_tablet=”0px” body_quote_text_shadow_vertical_length_tablet=”0px” body_quote_text_shadow_blur_strength_tablet=”1px” box_shadow_horizontal_tablet=”0px” box_shadow_vertical_tablet=”0px” box_shadow_blur_tablet=”40px” box_shadow_spread_tablet=”0px” box_shadow_horizontal_image_tablet=”0px” box_shadow_vertical_image_tablet=”0px” box_shadow_blur_image_tablet=”40px” box_shadow_spread_image_tablet=”0px” text_shadow_horizontal_length_tablet=”0px” text_shadow_vertical_length_tablet=”0px” text_shadow_blur_strength_tablet=”1px” global_colors_info=”{}”]<\/p>\n Roddam Narasimha, Sourabh S. Diwan, Subrahamanyam Duvvuri, K. R. Sreenivas and G. S. Bhat<\/strong>, 2011 \u201cLaboratory simulations show diabatic heating drives cumulus-cloud evolution and entrainment\u201d Proc. Natl. Acad. Sci. USA<\/em><\/strong>, 108(39)<\/strong>, 16164-16169. (Listed in \u201cThis Week in PNAS\u201d with a media summary entitled \u2018Laboratory cloud simulations reveal key role of internal heating\u2019<\/em>)<\/p>\n [\/et_pb_blurb][et_pb_blurb use_icon=”on” font_icon=”%%59%%” icon_color=”#bda392″ icon_placement=”left” image_icon_width=”27px” content_max_width=”900px” image_icon_width_last_edited=”on|phone” _builder_version=”4.18.0″ _module_preset=”default” header_font=”Nunito|700|||||||” header_font_size=”16px” body_font=”Nunito||||||||” body_font_size=”17px” body_link_text_color=”#727272″ vertical_offset_tablet=”0″ horizontal_offset_tablet=”0″ z_index_tablet=”0″ header_text_shadow_horizontal_length_tablet=”0px” header_text_shadow_vertical_length_tablet=”0px” header_text_shadow_blur_strength_tablet=”1px” body_text_shadow_horizontal_length_tablet=”0px” body_text_shadow_vertical_length_tablet=”0px” body_text_shadow_blur_strength_tablet=”1px” body_link_text_shadow_horizontal_length_tablet=”0px” body_link_text_shadow_vertical_length_tablet=”0px” body_link_text_shadow_blur_strength_tablet=”1px” body_ul_text_shadow_horizontal_length_tablet=”0px” body_ul_text_shadow_vertical_length_tablet=”0px” body_ul_text_shadow_blur_strength_tablet=”1px” body_ol_text_shadow_horizontal_length_tablet=”0px” body_ol_text_shadow_vertical_length_tablet=”0px” body_ol_text_shadow_blur_strength_tablet=”1px” body_quote_text_shadow_horizontal_length_tablet=”0px” body_quote_text_shadow_vertical_length_tablet=”0px” body_quote_text_shadow_blur_strength_tablet=”1px” box_shadow_horizontal_tablet=”0px” box_shadow_vertical_tablet=”0px” box_shadow_blur_tablet=”40px” box_shadow_spread_tablet=”0px” box_shadow_horizontal_image_tablet=”0px” box_shadow_vertical_image_tablet=”0px” box_shadow_blur_image_tablet=”40px” box_shadow_spread_image_tablet=”0px” text_shadow_horizontal_length_tablet=”0px” text_shadow_vertical_length_tablet=”0px” text_shadow_blur_strength_tablet=”1px” global_colors_info=”{}”]<\/p>\n Sourabh S. Diwan and O. N. Ramesh<\/strong>, 2009 \u201cOn the origin of the inflectional instability of a laminar separation bubble\u201d, J. Fluid Mech.<\/em>,<\/strong> 629<\/strong>, 263-298.<\/p>\n [\/et_pb_blurb][et_pb_blurb use_icon=”on” font_icon=”%%59%%” icon_color=”#bda392″ icon_placement=”left” image_icon_width=”27px” content_max_width=”900px” image_icon_width_last_edited=”on|phone” _builder_version=”4.18.0″ _module_preset=”default” header_font=”Nunito|700|||||||” header_font_size=”16px” body_font=”Nunito||||||||” body_font_size=”17px” body_link_text_color=”#727272″ vertical_offset_tablet=”0″ horizontal_offset_tablet=”0″ z_index_tablet=”0″ header_text_shadow_horizontal_length_tablet=”0px” header_text_shadow_vertical_length_tablet=”0px” header_text_shadow_blur_strength_tablet=”1px” body_text_shadow_horizontal_length_tablet=”0px” body_text_shadow_vertical_length_tablet=”0px” body_text_shadow_blur_strength_tablet=”1px” body_link_text_shadow_horizontal_length_tablet=”0px” body_link_text_shadow_vertical_length_tablet=”0px” body_link_text_shadow_blur_strength_tablet=”1px” body_ul_text_shadow_horizontal_length_tablet=”0px” body_ul_text_shadow_vertical_length_tablet=”0px” body_ul_text_shadow_blur_strength_tablet=”1px” body_ol_text_shadow_horizontal_length_tablet=”0px” body_ol_text_shadow_vertical_length_tablet=”0px” body_ol_text_shadow_blur_strength_tablet=”1px” body_quote_text_shadow_horizontal_length_tablet=”0px” body_quote_text_shadow_vertical_length_tablet=”0px” body_quote_text_shadow_blur_strength_tablet=”1px” box_shadow_horizontal_tablet=”0px” box_shadow_vertical_tablet=”0px” box_shadow_blur_tablet=”40px” box_shadow_spread_tablet=”0px” box_shadow_horizontal_image_tablet=”0px” box_shadow_vertical_image_tablet=”0px” box_shadow_blur_image_tablet=”40px” box_shadow_spread_image_tablet=”0px” text_shadow_horizontal_length_tablet=”0px” text_shadow_vertical_length_tablet=”0px” text_shadow_blur_strength_tablet=”1px” global_colors_info=”{}”]<\/p>\n Sourabh S. Diwan and O. N. Ramesh<\/strong>, 2007 \u201cLaminar separation bubbles: Dynamics and control\u201d, Sadhana<\/em> (Proceedings of Indian Academy of Sciences),<\/strong> 32<\/strong>, 103-109.<\/p>\n [\/et_pb_blurb][\/et_pb_column][\/et_pb_row][et_pb_row disabled_on=”on|on|on” _builder_version=”4.18.0″ background_size=”initial” background_position=”top_left” background_repeat=”repeat” disabled=”on” locked=”off” global_colors_info=”{}”][et_pb_column type=”4_4″ _builder_version=”4.16″ custom_padding=”|||” global_colors_info=”{}” custom_padding__hover=”|||”][et_pb_blurb use_icon=”on” font_icon=”%%59%%” icon_color=”#bda392″ icon_placement=”left” image_icon_width=”27px” content_max_width=”900px” image_icon_width_last_edited=”on|phone” _builder_version=”4.18.0″ _module_preset=”default” header_font=”Nunito|700|||||||” header_font_size=”16px” body_font=”Nunito||||||||” body_font_size=”17px” body_link_text_color=”#727272″ vertical_offset_tablet=”0″ horizontal_offset_tablet=”0″ z_index_tablet=”0″ header_text_shadow_horizontal_length_tablet=”0px” header_text_shadow_vertical_length_tablet=”0px” header_text_shadow_blur_strength_tablet=”1px” body_text_shadow_horizontal_length_tablet=”0px” body_text_shadow_vertical_length_tablet=”0px” body_text_shadow_blur_strength_tablet=”1px” body_link_text_shadow_horizontal_length_tablet=”0px” body_link_text_shadow_vertical_length_tablet=”0px” body_link_text_shadow_blur_strength_tablet=”1px” body_ul_text_shadow_horizontal_length_tablet=”0px” body_ul_text_shadow_vertical_length_tablet=”0px” body_ul_text_shadow_blur_strength_tablet=”1px” body_ol_text_shadow_horizontal_length_tablet=”0px” body_ol_text_shadow_vertical_length_tablet=”0px” body_ol_text_shadow_blur_strength_tablet=”1px” body_quote_text_shadow_horizontal_length_tablet=”0px” body_quote_text_shadow_vertical_length_tablet=”0px” body_quote_text_shadow_blur_strength_tablet=”1px” box_shadow_horizontal_tablet=”0px” box_shadow_vertical_tablet=”0px” box_shadow_blur_tablet=”40px” box_shadow_spread_tablet=”0px” box_shadow_horizontal_image_tablet=”0px” box_shadow_vertical_image_tablet=”0px” box_shadow_blur_image_tablet=”40px” box_shadow_spread_image_tablet=”0px” text_shadow_horizontal_length_tablet=”0px” text_shadow_vertical_length_tablet=”0px” text_shadow_blur_strength_tablet=”1px” global_colors_info=”{}”]<\/p>\n Rohit Singhal, S. Ravichandran, and Sourabh S. Diwan<\/strong>, 2022 \u201cDirect Numerical Simulation of a Moist Cough Flow using Eulerian Approximation for Liquid Droplets\u201d, Int. J. Comput. Fluid Dyn.,<\/em><\/strong> 35(9)<\/strong>, 778-797 (Invited article<\/em><\/strong> for a special issue on<\/em> \u201cCFD and COVID 19\u201d<\/em>)<\/p>\n [\/et_pb_blurb][et_pb_blurb use_icon=”on” font_icon=”%%59%%” icon_color=”#bda392″ icon_placement=”left” image_icon_width=”27px” content_max_width=”900px” image_icon_width_last_edited=”on|phone” _builder_version=”4.18.0″ _module_preset=”default” header_font=”Nunito|700|||||||” header_font_size=”16px” body_font=”Nunito||||||||” body_font_size=”17px” body_link_text_color=”#727272″ vertical_offset_tablet=”0″ horizontal_offset_tablet=”0″ z_index_tablet=”0″ header_text_shadow_horizontal_length_tablet=”0px” header_text_shadow_vertical_length_tablet=”0px” header_text_shadow_blur_strength_tablet=”1px” body_text_shadow_horizontal_length_tablet=”0px” body_text_shadow_vertical_length_tablet=”0px” body_text_shadow_blur_strength_tablet=”1px” body_link_text_shadow_horizontal_length_tablet=”0px” body_link_text_shadow_vertical_length_tablet=”0px” body_link_text_shadow_blur_strength_tablet=”1px” body_ul_text_shadow_horizontal_length_tablet=”0px” body_ul_text_shadow_vertical_length_tablet=”0px” body_ul_text_shadow_blur_strength_tablet=”1px” body_ol_text_shadow_horizontal_length_tablet=”0px” body_ol_text_shadow_vertical_length_tablet=”0px” body_ol_text_shadow_blur_strength_tablet=”1px” body_quote_text_shadow_horizontal_length_tablet=”0px” body_quote_text_shadow_vertical_length_tablet=”0px” body_quote_text_shadow_blur_strength_tablet=”1px” box_shadow_horizontal_tablet=”0px” box_shadow_vertical_tablet=”0px” box_shadow_blur_tablet=”40px” box_shadow_spread_tablet=”0px” box_shadow_horizontal_image_tablet=”0px” box_shadow_vertical_image_tablet=”0px” box_shadow_blur_image_tablet=”40px” box_shadow_spread_image_tablet=”0px” text_shadow_horizontal_length_tablet=”0px” text_shadow_vertical_length_tablet=”0px” text_shadow_blur_strength_tablet=”1px” global_colors_info=”{}”]<\/p>\n A.B. Aadhishwaran and Sourabh S. Diwan<\/strong>, 2021 \u201cPredominance of pressure transport in spatial energy budget for a mixing layer approaching absolute instability\u201d, Phys. Rev. Fluids<\/em><\/strong>, 6<\/strong>, L091901<\/p>\n [\/et_pb_blurb][et_pb_blurb use_icon=”on” font_icon=”%%59%%” icon_color=”#bda392″ icon_placement=”left” image_icon_width=”27px” content_max_width=”900px” image_icon_width_last_edited=”on|phone” _builder_version=”4.18.0″ _module_preset=”default” header_font=”Nunito|700|||||||” header_font_size=”16px” body_font=”Nunito||||||||” body_font_size=”17px” body_link_text_color=”#727272″ vertical_offset_tablet=”0″ horizontal_offset_tablet=”0″ z_index_tablet=”0″ header_text_shadow_horizontal_length_tablet=”0px” header_text_shadow_vertical_length_tablet=”0px” header_text_shadow_blur_strength_tablet=”1px” body_text_shadow_horizontal_length_tablet=”0px” body_text_shadow_vertical_length_tablet=”0px” body_text_shadow_blur_strength_tablet=”1px” body_link_text_shadow_horizontal_length_tablet=”0px” body_link_text_shadow_vertical_length_tablet=”0px” body_link_text_shadow_blur_strength_tablet=”1px” body_ul_text_shadow_horizontal_length_tablet=”0px” body_ul_text_shadow_vertical_length_tablet=”0px” body_ul_text_shadow_blur_strength_tablet=”1px” body_ol_text_shadow_horizontal_length_tablet=”0px” body_ol_text_shadow_vertical_length_tablet=”0px” body_ol_text_shadow_blur_strength_tablet=”1px” body_quote_text_shadow_horizontal_length_tablet=”0px” body_quote_text_shadow_vertical_length_tablet=”0px” body_quote_text_shadow_blur_strength_tablet=”1px” box_shadow_horizontal_tablet=”0px” box_shadow_vertical_tablet=”0px” box_shadow_blur_tablet=”40px” box_shadow_spread_tablet=”0px” box_shadow_horizontal_image_tablet=”0px” box_shadow_vertical_image_tablet=”0px” box_shadow_blur_image_tablet=”40px” box_shadow_spread_image_tablet=”0px” text_shadow_horizontal_length_tablet=”0px” text_shadow_vertical_length_tablet=”0px” text_shadow_blur_strength_tablet=”1px” global_colors_info=”{}”]<\/p>\n A. Samson, Karthik Naicker and Sourabh S. Diwan<\/strong>, 2021 \u201cInstability mechanisms and intermittency distribution in adverse pressure gradient attached and separated boundary layers\u201d, Phys. Fluids<\/em><\/strong>, 33<\/strong>, 094106 (Invited article<\/em><\/strong>: Special Topic on Tribute to Frank M. White on his 88th anniversary<\/em>)<\/p>\n [\/et_pb_blurb][et_pb_blurb use_icon=”on” font_icon=”%%59%%” icon_color=”#bda392″ icon_placement=”left” image_icon_width=”27px” content_max_width=”900px” image_icon_width_last_edited=”on|phone” _builder_version=”4.18.0″ _module_preset=”default” header_font=”Nunito|700|||||||” header_font_size=”16px” body_font=”Nunito||||||||” body_font_size=”17px” body_link_text_color=”#727272″ vertical_offset_tablet=”0″ horizontal_offset_tablet=”0″ z_index_tablet=”0″ header_text_shadow_horizontal_length_tablet=”0px” header_text_shadow_vertical_length_tablet=”0px” header_text_shadow_blur_strength_tablet=”1px” body_text_shadow_horizontal_length_tablet=”0px” body_text_shadow_vertical_length_tablet=”0px” body_text_shadow_blur_strength_tablet=”1px” body_link_text_shadow_horizontal_length_tablet=”0px” body_link_text_shadow_vertical_length_tablet=”0px” body_link_text_shadow_blur_strength_tablet=”1px” body_ul_text_shadow_horizontal_length_tablet=”0px” body_ul_text_shadow_vertical_length_tablet=”0px” body_ul_text_shadow_blur_strength_tablet=”1px” body_ol_text_shadow_horizontal_length_tablet=”0px” body_ol_text_shadow_vertical_length_tablet=”0px” body_ol_text_shadow_blur_strength_tablet=”1px” body_quote_text_shadow_horizontal_length_tablet=”0px” body_quote_text_shadow_vertical_length_tablet=”0px” body_quote_text_shadow_blur_strength_tablet=”1px” box_shadow_horizontal_tablet=”0px” box_shadow_vertical_tablet=”0px” box_shadow_blur_tablet=”40px” box_shadow_spread_tablet=”0px” box_shadow_horizontal_image_tablet=”0px” box_shadow_vertical_image_tablet=”0px” box_shadow_blur_image_tablet=”40px” box_shadow_spread_image_tablet=”0px” text_shadow_horizontal_length_tablet=”0px” text_shadow_vertical_length_tablet=”0px” text_shadow_blur_strength_tablet=”1px” global_colors_info=”{}”]<\/p>\n Srinivas Kirthy K. and Sourabh S. Diwan<\/strong>, 2021 \u201cEnergy budget analysis and neutral curve characteristics for the linear instability of Couette\u2013Poiseuille flow\u201d, Phys. Fluids<\/em><\/strong>, 33<\/strong>, 034102.<\/p>\n [\/et_pb_blurb][et_pb_blurb use_icon=”on” font_icon=”%%59%%” icon_color=”#bda392″ icon_placement=”left” image_icon_width=”27px” content_max_width=”900px” image_icon_width_last_edited=”on|phone” _builder_version=”4.18.0″ _module_preset=”default” header_font=”Nunito|700|||||||” header_font_size=”16px” body_font=”Nunito||||||||” body_font_size=”17px” body_link_text_color=”#727272″ vertical_offset_tablet=”0″ horizontal_offset_tablet=”0″ z_index_tablet=”0″ header_text_shadow_horizontal_length_tablet=”0px” header_text_shadow_vertical_length_tablet=”0px” header_text_shadow_blur_strength_tablet=”1px” body_text_shadow_horizontal_length_tablet=”0px” body_text_shadow_vertical_length_tablet=”0px” body_text_shadow_blur_strength_tablet=”1px” body_link_text_shadow_horizontal_length_tablet=”0px” body_link_text_shadow_vertical_length_tablet=”0px” body_link_text_shadow_blur_strength_tablet=”1px” body_ul_text_shadow_horizontal_length_tablet=”0px” body_ul_text_shadow_vertical_length_tablet=”0px” body_ul_text_shadow_blur_strength_tablet=”1px” body_ol_text_shadow_horizontal_length_tablet=”0px” body_ol_text_shadow_vertical_length_tablet=”0px” body_ol_text_shadow_blur_strength_tablet=”1px” body_quote_text_shadow_horizontal_length_tablet=”0px” body_quote_text_shadow_vertical_length_tablet=”0px” body_quote_text_shadow_blur_strength_tablet=”1px” box_shadow_horizontal_tablet=”0px” box_shadow_vertical_tablet=”0px” box_shadow_blur_tablet=”40px” box_shadow_spread_tablet=”0px” box_shadow_horizontal_image_tablet=”0px” box_shadow_vertical_image_tablet=”0px” box_shadow_blur_image_tablet=”40px” box_shadow_spread_image_tablet=”0px” text_shadow_horizontal_length_tablet=”0px” text_shadow_vertical_length_tablet=”0px” text_shadow_blur_strength_tablet=”1px” global_colors_info=”{}”]<\/p>\n Sourabh S. Diwan and Jonathan F. Morrison<\/strong>, 2021 \u201cIntermediate Scaling and Logarithmic Invariance in Turbulent Pipe Flow\u201d, J. Fluid Mech.<\/em>,<\/strong> 913<\/strong>, R1.<\/p>\n [\/et_pb_blurb][et_pb_blurb use_icon=”on” font_icon=”%%59%%” icon_color=”#bda392″ icon_placement=”left” image_icon_width=”27px” content_max_width=”900px” image_icon_width_last_edited=”on|phone” _builder_version=”4.18.0″ _module_preset=”default” header_font=”Nunito|700|||||||” header_font_size=”16px” body_font=”Nunito||||||||” body_font_size=”17px” body_link_text_color=”#727272″ vertical_offset_tablet=”0″ horizontal_offset_tablet=”0″ z_index_tablet=”0″ header_text_shadow_horizontal_length_tablet=”0px” header_text_shadow_vertical_length_tablet=”0px” header_text_shadow_blur_strength_tablet=”1px” body_text_shadow_horizontal_length_tablet=”0px” body_text_shadow_vertical_length_tablet=”0px” body_text_shadow_blur_strength_tablet=”1px” body_link_text_shadow_horizontal_length_tablet=”0px” body_link_text_shadow_vertical_length_tablet=”0px” body_link_text_shadow_blur_strength_tablet=”1px” body_ul_text_shadow_horizontal_length_tablet=”0px” body_ul_text_shadow_vertical_length_tablet=”0px” body_ul_text_shadow_blur_strength_tablet=”1px” body_ol_text_shadow_horizontal_length_tablet=”0px” body_ol_text_shadow_vertical_length_tablet=”0px” body_ol_text_shadow_blur_strength_tablet=”1px” body_quote_text_shadow_horizontal_length_tablet=”0px” body_quote_text_shadow_vertical_length_tablet=”0px” body_quote_text_shadow_blur_strength_tablet=”1px” box_shadow_horizontal_tablet=”0px” box_shadow_vertical_tablet=”0px” box_shadow_blur_tablet=”40px” box_shadow_spread_tablet=”0px” box_shadow_horizontal_image_tablet=”0px” box_shadow_vertical_image_tablet=”0px” box_shadow_blur_image_tablet=”40px” box_shadow_spread_image_tablet=”0px” text_shadow_horizontal_length_tablet=”0px” text_shadow_vertical_length_tablet=”0px” text_shadow_blur_strength_tablet=”1px” global_colors_info=”{}”]<\/p>\n Sourabh S. Diwan, S. Ravichandran, Rama Govindarajan, Roddam Narasimha<\/strong>, 2020 \u201cUnderstanding Transmission Dynamics of COVID\u201119\u2011Type Infections by Direct Numerical Simulations of Cough\/Sneeze Flows\u201d, Trans. Indian Natl. Acad. Eng.<\/em><\/strong>, June-3<\/strong>, 1-7.<\/p>\n [\/et_pb_blurb][et_pb_blurb use_icon=”on” font_icon=”%%59%%” icon_color=”#bda392″ icon_placement=”left” image_icon_width=”27px” content_max_width=”900px” image_icon_width_last_edited=”on|phone” _builder_version=”4.18.0″ _module_preset=”default” header_font=”Nunito|700|||||||” header_font_size=”16px” body_font=”Nunito||||||||” body_font_size=”17px” body_link_text_color=”#727272″ vertical_offset_tablet=”0″ horizontal_offset_tablet=”0″ z_index_tablet=”0″ header_text_shadow_horizontal_length_tablet=”0px” header_text_shadow_vertical_length_tablet=”0px” header_text_shadow_blur_strength_tablet=”1px” body_text_shadow_horizontal_length_tablet=”0px” body_text_shadow_vertical_length_tablet=”0px” body_text_shadow_blur_strength_tablet=”1px” body_link_text_shadow_horizontal_length_tablet=”0px” body_link_text_shadow_vertical_length_tablet=”0px” body_link_text_shadow_blur_strength_tablet=”1px” body_ul_text_shadow_horizontal_length_tablet=”0px” body_ul_text_shadow_vertical_length_tablet=”0px” body_ul_text_shadow_blur_strength_tablet=”1px” body_ol_text_shadow_horizontal_length_tablet=”0px” body_ol_text_shadow_vertical_length_tablet=”0px” body_ol_text_shadow_blur_strength_tablet=”1px” body_quote_text_shadow_horizontal_length_tablet=”0px” body_quote_text_shadow_vertical_length_tablet=”0px” body_quote_text_shadow_blur_strength_tablet=”1px” box_shadow_horizontal_tablet=”0px” box_shadow_vertical_tablet=”0px” box_shadow_blur_tablet=”40px” box_shadow_spread_tablet=”0px” box_shadow_horizontal_image_tablet=”0px” box_shadow_vertical_image_tablet=”0px” box_shadow_blur_image_tablet=”40px” box_shadow_spread_image_tablet=”0px” text_shadow_horizontal_length_tablet=”0px” text_shadow_vertical_length_tablet=”0px” text_shadow_blur_strength_tablet=”1px” global_colors_info=”{}”]<\/p>\n Aditya Anand and Sourabh S. Diwan, <\/strong>2020 \u201cTime\u2011frequency analysis for two cases of boundary\u2011layer transition induced by random distributed roughness\u201d, Exp. Fluids<\/em><\/strong>, 61<\/strong>:60.<\/p>\n [\/et_pb_blurb][et_pb_blurb use_icon=”on” font_icon=”%%59%%” icon_color=”#bda392″ icon_placement=”left” image_icon_width=”27px” content_max_width=”900px” image_icon_width_last_edited=”on|phone” _builder_version=”4.18.0″ _module_preset=”default” header_font=”Nunito|700|||||||” header_font_size=”16px” body_font=”Nunito||||||||” body_font_size=”17px” body_link_text_color=”#727272″ vertical_offset_tablet=”0″ horizontal_offset_tablet=”0″ z_index_tablet=”0″ header_text_shadow_horizontal_length_tablet=”0px” header_text_shadow_vertical_length_tablet=”0px” header_text_shadow_blur_strength_tablet=”1px” body_text_shadow_horizontal_length_tablet=”0px” body_text_shadow_vertical_length_tablet=”0px” body_text_shadow_blur_strength_tablet=”1px” body_link_text_shadow_horizontal_length_tablet=”0px” body_link_text_shadow_vertical_length_tablet=”0px” body_link_text_shadow_blur_strength_tablet=”1px” body_ul_text_shadow_horizontal_length_tablet=”0px” body_ul_text_shadow_vertical_length_tablet=”0px” body_ul_text_shadow_blur_strength_tablet=”1px” body_ol_text_shadow_horizontal_length_tablet=”0px” body_ol_text_shadow_vertical_length_tablet=”0px” body_ol_text_shadow_blur_strength_tablet=”1px” body_quote_text_shadow_horizontal_length_tablet=”0px” body_quote_text_shadow_vertical_length_tablet=”0px” body_quote_text_shadow_blur_strength_tablet=”1px” box_shadow_horizontal_tablet=”0px” box_shadow_vertical_tablet=”0px” box_shadow_blur_tablet=”40px” box_shadow_spread_tablet=”0px” box_shadow_horizontal_image_tablet=”0px” box_shadow_vertical_image_tablet=”0px” box_shadow_blur_image_tablet=”40px” box_shadow_spread_image_tablet=”0px” text_shadow_horizontal_length_tablet=”0px” text_shadow_vertical_length_tablet=”0px” text_shadow_blur_strength_tablet=”1px” global_colors_info=”{}”]<\/p>\n Sourabh S. Diwan and Jonathan F. Morrison<\/strong>, 2017 \u201cSpectral structure and linear mechanisms in a rapidly-distorted boundary layer\u201d, Int. J. Heat Fluid Flow<\/em><\/strong>, 67<\/strong>, 63-73. (Invited article for the special issue<\/em><\/strong>: Symposium on Experiments and Simulations in Fluid Dynamics Research<\/em>)<\/p>\n [\/et_pb_blurb][et_pb_blurb use_icon=”on” font_icon=”%%59%%” icon_color=”#bda392″ icon_placement=”left” image_icon_width=”27px” content_max_width=”900px” image_icon_width_last_edited=”on|phone” _builder_version=”4.18.0″ _module_preset=”default” header_font=”Nunito|700|||||||” header_font_size=”16px” body_font=”Nunito||||||||” body_font_size=”17px” body_link_text_color=”#727272″ vertical_offset_tablet=”0″ horizontal_offset_tablet=”0″ z_index_tablet=”0″ header_text_shadow_horizontal_length_tablet=”0px” header_text_shadow_vertical_length_tablet=”0px” header_text_shadow_blur_strength_tablet=”1px” body_text_shadow_horizontal_length_tablet=”0px” body_text_shadow_vertical_length_tablet=”0px” body_text_shadow_blur_strength_tablet=”1px” body_link_text_shadow_horizontal_length_tablet=”0px” body_link_text_shadow_vertical_length_tablet=”0px” body_link_text_shadow_blur_strength_tablet=”1px” body_ul_text_shadow_horizontal_length_tablet=”0px” body_ul_text_shadow_vertical_length_tablet=”0px” body_ul_text_shadow_blur_strength_tablet=”1px” body_ol_text_shadow_horizontal_length_tablet=”0px” body_ol_text_shadow_vertical_length_tablet=”0px” body_ol_text_shadow_blur_strength_tablet=”1px” body_quote_text_shadow_horizontal_length_tablet=”0px” body_quote_text_shadow_vertical_length_tablet=”0px” body_quote_text_shadow_blur_strength_tablet=”1px” box_shadow_horizontal_tablet=”0px” box_shadow_vertical_tablet=”0px” box_shadow_blur_tablet=”40px” box_shadow_spread_tablet=”0px” box_shadow_horizontal_image_tablet=”0px” box_shadow_vertical_image_tablet=”0px” box_shadow_blur_image_tablet=”40px” box_shadow_spread_image_tablet=”0px” text_shadow_horizontal_length_tablet=”0px” text_shadow_vertical_length_tablet=”0px” text_shadow_blur_strength_tablet=”1px” global_colors_info=”{}”]<\/p>\n Sourabh S. Diwan<\/strong>, 2015 \u201cNecessary conditions for spatial inviscid instability\u201d, Proc. Roy. Soc. A<\/em><\/strong>, 471<\/strong>, 20140607.<\/p>\n [\/et_pb_blurb][et_pb_blurb use_icon=”on” font_icon=”%%59%%” icon_color=”#bda392″ icon_placement=”left” image_icon_width=”27px” content_max_width=”900px” image_icon_width_last_edited=”on|phone” _builder_version=”4.18.0″ _module_preset=”default” header_font=”Nunito|700|||||||” header_font_size=”16px” body_font=”Nunito||||||||” body_font_size=”17px” body_link_text_color=”#727272″ vertical_offset_tablet=”0″ horizontal_offset_tablet=”0″ z_index_tablet=”0″ header_text_shadow_horizontal_length_tablet=”0px” header_text_shadow_vertical_length_tablet=”0px” header_text_shadow_blur_strength_tablet=”1px” body_text_shadow_horizontal_length_tablet=”0px” body_text_shadow_vertical_length_tablet=”0px” body_text_shadow_blur_strength_tablet=”1px” body_link_text_shadow_horizontal_length_tablet=”0px” body_link_text_shadow_vertical_length_tablet=”0px” body_link_text_shadow_blur_strength_tablet=”1px” body_ul_text_shadow_horizontal_length_tablet=”0px” body_ul_text_shadow_vertical_length_tablet=”0px” body_ul_text_shadow_blur_strength_tablet=”1px” body_ol_text_shadow_horizontal_length_tablet=”0px” body_ol_text_shadow_vertical_length_tablet=”0px” body_ol_text_shadow_blur_strength_tablet=”1px” body_quote_text_shadow_horizontal_length_tablet=”0px” body_quote_text_shadow_vertical_length_tablet=”0px” body_quote_text_shadow_blur_strength_tablet=”1px” box_shadow_horizontal_tablet=”0px” box_shadow_vertical_tablet=”0px” box_shadow_blur_tablet=”40px” box_shadow_spread_tablet=”0px” box_shadow_horizontal_image_tablet=”0px” box_shadow_vertical_image_tablet=”0px” box_shadow_blur_image_tablet=”40px” box_shadow_spread_image_tablet=”0px” text_shadow_horizontal_length_tablet=”0px” text_shadow_vertical_length_tablet=”0px” text_shadow_blur_strength_tablet=”1px” global_colors_info=”{}”]<\/p>\n Sourabh S. Diwan, P. Prasanth, K. R. Sreenivas, S. M. Deshpande and Roddam Narasimha<\/strong>, 2014 \u201cCumulus-type flows in the laboratory and on the computer: simulating cloud form, evolution and large-scale structure\u201d, Bull. Amer. Meteor. Soc<\/em>.,<\/strong> 95(10)<\/strong>, 1541-1548. (Selected under \u2018In Box\u2019 section meant for articles with \u2018Insights and Innovations<\/em>\u2019).<\/p>\n [\/et_pb_blurb][et_pb_blurb use_icon=”on” font_icon=”%%59%%” icon_color=”#bda392″ icon_placement=”left” image_icon_width=”27px” content_max_width=”900px” image_icon_width_last_edited=”on|phone” _builder_version=”4.18.0″ _module_preset=”default” header_font=”Nunito|700|||||||” header_font_size=”16px” body_font=”Nunito||||||||” body_font_size=”17px” body_link_text_color=”#727272″ vertical_offset_tablet=”0″ horizontal_offset_tablet=”0″ z_index_tablet=”0″ header_text_shadow_horizontal_length_tablet=”0px” header_text_shadow_vertical_length_tablet=”0px” header_text_shadow_blur_strength_tablet=”1px” body_text_shadow_horizontal_length_tablet=”0px” body_text_shadow_vertical_length_tablet=”0px” body_text_shadow_blur_strength_tablet=”1px” body_link_text_shadow_horizontal_length_tablet=”0px” body_link_text_shadow_vertical_length_tablet=”0px” body_link_text_shadow_blur_strength_tablet=”1px” body_ul_text_shadow_horizontal_length_tablet=”0px” body_ul_text_shadow_vertical_length_tablet=”0px” body_ul_text_shadow_blur_strength_tablet=”1px” body_ol_text_shadow_horizontal_length_tablet=”0px” body_ol_text_shadow_vertical_length_tablet=”0px” body_ol_text_shadow_blur_strength_tablet=”1px” body_quote_text_shadow_horizontal_length_tablet=”0px” body_quote_text_shadow_vertical_length_tablet=”0px” body_quote_text_shadow_blur_strength_tablet=”1px” box_shadow_horizontal_tablet=”0px” box_shadow_vertical_tablet=”0px” box_shadow_blur_tablet=”40px” box_shadow_spread_tablet=”0px” box_shadow_horizontal_image_tablet=”0px” box_shadow_vertical_image_tablet=”0px” box_shadow_blur_image_tablet=”40px” box_shadow_spread_image_tablet=”0px” text_shadow_horizontal_length_tablet=”0px” text_shadow_vertical_length_tablet=”0px” text_shadow_blur_strength_tablet=”1px” global_colors_info=”{}”]<\/p>\n Sourabh S. Diwan and O. N. Ramesh<\/strong>, 2012 \u201cRelevance of local parallel theory to the linear stability of laminar separation bubbles\u201d J. Fluid Mech.<\/em>,<\/strong> 698<\/strong>, 468-478.<\/p>\n [\/et_pb_blurb][et_pb_blurb use_icon=”on” font_icon=”%%59%%” icon_color=”#bda392″ icon_placement=”left” image_icon_width=”27px” content_max_width=”900px” image_icon_width_last_edited=”on|phone” _builder_version=”4.18.0″ _module_preset=”default” header_font=”Nunito|700|||||||” header_font_size=”16px” body_font=”Nunito||||||||” body_font_size=”17px” body_link_text_color=”#727272″ vertical_offset_tablet=”0″ horizontal_offset_tablet=”0″ z_index_tablet=”0″ header_text_shadow_horizontal_length_tablet=”0px” header_text_shadow_vertical_length_tablet=”0px” header_text_shadow_blur_strength_tablet=”1px” body_text_shadow_horizontal_length_tablet=”0px” body_text_shadow_vertical_length_tablet=”0px” body_text_shadow_blur_strength_tablet=”1px” body_link_text_shadow_horizontal_length_tablet=”0px” body_link_text_shadow_vertical_length_tablet=”0px” body_link_text_shadow_blur_strength_tablet=”1px” body_ul_text_shadow_horizontal_length_tablet=”0px” body_ul_text_shadow_vertical_length_tablet=”0px” body_ul_text_shadow_blur_strength_tablet=”1px” body_ol_text_shadow_horizontal_length_tablet=”0px” body_ol_text_shadow_vertical_length_tablet=”0px” body_ol_text_shadow_blur_strength_tablet=”1px” body_quote_text_shadow_horizontal_length_tablet=”0px” body_quote_text_shadow_vertical_length_tablet=”0px” body_quote_text_shadow_blur_strength_tablet=”1px” box_shadow_horizontal_tablet=”0px” box_shadow_vertical_tablet=”0px” box_shadow_blur_tablet=”40px” box_shadow_spread_tablet=”0px” box_shadow_horizontal_image_tablet=”0px” box_shadow_vertical_image_tablet=”0px” box_shadow_blur_image_tablet=”40px” box_shadow_spread_image_tablet=”0px” text_shadow_horizontal_length_tablet=”0px” text_shadow_vertical_length_tablet=”0px” text_shadow_blur_strength_tablet=”1px” global_colors_info=”{}”]<\/p>\n Sourabh S. Diwan, Roddam Narasimha, G. S. Bhat and K. R. Sreenivas<\/strong>, 2011 \u201cLaboratory studies of anomalous entrainment in cumulus cloud flows\u201d J. Phys.: Conf. Series<\/em><\/strong>, 318<\/strong>, 072014.<\/p>\n [\/et_pb_blurb][et_pb_blurb use_icon=”on” font_icon=”%%59%%” icon_color=”#bda392″ icon_placement=”left” image_icon_width=”27px” content_max_width=”900px” image_icon_width_last_edited=”on|phone” _builder_version=”4.18.0″ _module_preset=”default” header_font=”Nunito|700|||||||” header_font_size=”16px” body_font=”Nunito||||||||” body_font_size=”17px” body_link_text_color=”#727272″ vertical_offset_tablet=”0″ horizontal_offset_tablet=”0″ z_index_tablet=”0″ header_text_shadow_horizontal_length_tablet=”0px” header_text_shadow_vertical_length_tablet=”0px” header_text_shadow_blur_strength_tablet=”1px” body_text_shadow_horizontal_length_tablet=”0px” body_text_shadow_vertical_length_tablet=”0px” body_text_shadow_blur_strength_tablet=”1px” body_link_text_shadow_horizontal_length_tablet=”0px” body_link_text_shadow_vertical_length_tablet=”0px” body_link_text_shadow_blur_strength_tablet=”1px” body_ul_text_shadow_horizontal_length_tablet=”0px” body_ul_text_shadow_vertical_length_tablet=”0px” body_ul_text_shadow_blur_strength_tablet=”1px” body_ol_text_shadow_horizontal_length_tablet=”0px” body_ol_text_shadow_vertical_length_tablet=”0px” body_ol_text_shadow_blur_strength_tablet=”1px” body_quote_text_shadow_horizontal_length_tablet=”0px” body_quote_text_shadow_vertical_length_tablet=”0px” body_quote_text_shadow_blur_strength_tablet=”1px” box_shadow_horizontal_tablet=”0px” box_shadow_vertical_tablet=”0px” box_shadow_blur_tablet=”40px” box_shadow_spread_tablet=”0px” box_shadow_horizontal_image_tablet=”0px” box_shadow_vertical_image_tablet=”0px” box_shadow_blur_image_tablet=”40px” box_shadow_spread_image_tablet=”0px” text_shadow_horizontal_length_tablet=”0px” text_shadow_vertical_length_tablet=”0px” text_shadow_blur_strength_tablet=”1px” global_colors_info=”{}”]<\/p>\n Roddam Narasimha, Sourabh S. Diwan, Subrahamanyam Duvvuri, K. R. Sreenivas and G. S. Bhat<\/strong>, 2011 \u201cLaboratory simulations show diabatic heating drives cumulus-cloud evolution and entrainment\u201d Proc. Natl. Acad. Sci. USA<\/em><\/strong>, 108(39)<\/strong>, 16164-16169. (Listed in \u201cThis Week in PNAS\u201d with a media summary entitled \u2018Laboratory cloud simulations reveal key role of internal heating\u2019<\/em>)<\/p>\n [\/et_pb_blurb][et_pb_blurb use_icon=”on” font_icon=”%%59%%” icon_color=”#bda392″ icon_placement=”left” image_icon_width=”27px” content_max_width=”900px” image_icon_width_last_edited=”on|phone” _builder_version=”4.18.0″ _module_preset=”default” header_font=”Nunito|700|||||||” header_font_size=”16px” body_font=”Nunito||||||||” body_font_size=”17px” body_link_text_color=”#727272″ vertical_offset_tablet=”0″ horizontal_offset_tablet=”0″ z_index_tablet=”0″ header_text_shadow_horizontal_length_tablet=”0px” header_text_shadow_vertical_length_tablet=”0px” header_text_shadow_blur_strength_tablet=”1px” body_text_shadow_horizontal_length_tablet=”0px” body_text_shadow_vertical_length_tablet=”0px” body_text_shadow_blur_strength_tablet=”1px” body_link_text_shadow_horizontal_length_tablet=”0px” body_link_text_shadow_vertical_length_tablet=”0px” body_link_text_shadow_blur_strength_tablet=”1px” body_ul_text_shadow_horizontal_length_tablet=”0px” body_ul_text_shadow_vertical_length_tablet=”0px” body_ul_text_shadow_blur_strength_tablet=”1px” body_ol_text_shadow_horizontal_length_tablet=”0px” body_ol_text_shadow_vertical_length_tablet=”0px” body_ol_text_shadow_blur_strength_tablet=”1px” body_quote_text_shadow_horizontal_length_tablet=”0px” body_quote_text_shadow_vertical_length_tablet=”0px” body_quote_text_shadow_blur_strength_tablet=”1px” box_shadow_horizontal_tablet=”0px” box_shadow_vertical_tablet=”0px” box_shadow_blur_tablet=”40px” box_shadow_spread_tablet=”0px” box_shadow_horizontal_image_tablet=”0px” box_shadow_vertical_image_tablet=”0px” box_shadow_blur_image_tablet=”40px” box_shadow_spread_image_tablet=”0px” text_shadow_horizontal_length_tablet=”0px” text_shadow_vertical_length_tablet=”0px” text_shadow_blur_strength_tablet=”1px” global_colors_info=”{}”]<\/p>\n Sourabh S. Diwan and O. N. Ramesh<\/strong>, 2009 \u201cOn the origin of the inflectional instability of a laminar separation bubble\u201d, J. Fluid Mech.<\/em>,<\/strong> 629<\/strong>, 263-298.<\/p>\n [\/et_pb_blurb][et_pb_blurb use_icon=”on” font_icon=”%%59%%” icon_color=”#bda392″ icon_placement=”left” image_icon_width=”27px” content_max_width=”900px” image_icon_width_last_edited=”on|phone” _builder_version=”4.18.0″ _module_preset=”default” header_font=”Nunito|700|||||||” header_font_size=”16px” body_font=”Nunito||||||||” body_font_size=”17px” body_link_text_color=”#727272″ vertical_offset_tablet=”0″ horizontal_offset_tablet=”0″ z_index_tablet=”0″ header_text_shadow_horizontal_length_tablet=”0px” header_text_shadow_vertical_length_tablet=”0px” header_text_shadow_blur_strength_tablet=”1px” body_text_shadow_horizontal_length_tablet=”0px” body_text_shadow_vertical_length_tablet=”0px” body_text_shadow_blur_strength_tablet=”1px” body_link_text_shadow_horizontal_length_tablet=”0px” body_link_text_shadow_vertical_length_tablet=”0px” body_link_text_shadow_blur_strength_tablet=”1px” body_ul_text_shadow_horizontal_length_tablet=”0px” body_ul_text_shadow_vertical_length_tablet=”0px” body_ul_text_shadow_blur_strength_tablet=”1px” body_ol_text_shadow_horizontal_length_tablet=”0px” body_ol_text_shadow_vertical_length_tablet=”0px” body_ol_text_shadow_blur_strength_tablet=”1px” body_quote_text_shadow_horizontal_length_tablet=”0px” body_quote_text_shadow_vertical_length_tablet=”0px” body_quote_text_shadow_blur_strength_tablet=”1px” box_shadow_horizontal_tablet=”0px” box_shadow_vertical_tablet=”0px” box_shadow_blur_tablet=”40px” box_shadow_spread_tablet=”0px” box_shadow_horizontal_image_tablet=”0px” box_shadow_vertical_image_tablet=”0px” box_shadow_blur_image_tablet=”40px” box_shadow_spread_image_tablet=”0px” text_shadow_horizontal_length_tablet=”0px” text_shadow_vertical_length_tablet=”0px” text_shadow_blur_strength_tablet=”1px” global_colors_info=”{}”]<\/p>\n Sourabh S. Diwan and O. N. Ramesh<\/strong>, 2007 \u201cLaminar separation bubbles: Dynamics and control\u201d, Sadhana<\/em> (Proceedings of Indian Academy of Sciences),<\/strong> 32<\/strong>, 103-109.<\/p>\n [\/et_pb_blurb][\/et_pb_column][\/et_pb_row][et_pb_row _builder_version=”4.18.0″ _module_preset=”default” global_colors_info=”{}”][et_pb_column type=”4_4″ _builder_version=”4.18.0″ _module_preset=”default” global_colors_info=”{}”][et_pb_blurb title=”Journal Papers (published\/accepted)” use_icon=”on” font_icon=”\||divi||400″ icon_color=”#bda392″ icon_placement=”left” image_icon_width=”27px” content_max_width=”1100px” _builder_version=”4.18.0″ _module_preset=”default” header_font=”Nunito||||||||” header_font_size=”24px” body_font=”Nunito||||||||” body_text_align=”left” body_font_size=”18px” image_icon_custom_margin=”||||false|false” image_icon_custom_padding=”||||false|false” module_alignment=”center” custom_margin=”||||false|false” animation_direction=”top” global_colors_info=”{}”]<\/p>\n [\/et_pb_blurb][et_pb_text _builder_version=”4.18.0″ _module_preset=”default” text_font=”Nunito||||||||” text_font_size=”17px” custom_margin=”||-43px|||” custom_padding=”||87px|||” animation_direction=”top” global_colors_info=”{}” background_pattern_color=”rgba(0,0,0,0.2)” background_mask_color=”#ffffff” text_text_shadow_horizontal_length=”text_text_shadow_style,%91object Object%93″ text_text_shadow_horizontal_length_tablet=”0px” text_text_shadow_vertical_length=”text_text_shadow_style,%91object Object%93″ text_text_shadow_vertical_length_tablet=”0px” text_text_shadow_blur_strength=”text_text_shadow_style,%91object Object%93″ text_text_shadow_blur_strength_tablet=”1px” link_text_shadow_horizontal_length=”link_text_shadow_style,%91object Object%93″ link_text_shadow_horizontal_length_tablet=”0px” link_text_shadow_vertical_length=”link_text_shadow_style,%91object Object%93″ link_text_shadow_vertical_length_tablet=”0px” link_text_shadow_blur_strength=”link_text_shadow_style,%91object Object%93″ link_text_shadow_blur_strength_tablet=”1px” ul_text_shadow_horizontal_length=”ul_text_shadow_style,%91object Object%93″ ul_text_shadow_horizontal_length_tablet=”0px” ul_text_shadow_vertical_length=”ul_text_shadow_style,%91object Object%93″ ul_text_shadow_vertical_length_tablet=”0px” ul_text_shadow_blur_strength=”ul_text_shadow_style,%91object Object%93″ ul_text_shadow_blur_strength_tablet=”1px” ol_text_shadow_horizontal_length=”ol_text_shadow_style,%91object Object%93″ ol_text_shadow_horizontal_length_tablet=”0px” ol_text_shadow_vertical_length=”ol_text_shadow_style,%91object Object%93″ ol_text_shadow_vertical_length_tablet=”0px” ol_text_shadow_blur_strength=”ol_text_shadow_style,%91object Object%93″ ol_text_shadow_blur_strength_tablet=”1px” quote_text_shadow_horizontal_length=”quote_text_shadow_style,%91object Object%93″ quote_text_shadow_horizontal_length_tablet=”0px” quote_text_shadow_vertical_length=”quote_text_shadow_style,%91object Object%93″ quote_text_shadow_vertical_length_tablet=”0px” quote_text_shadow_blur_strength=”quote_text_shadow_style,%91object Object%93″ quote_text_shadow_blur_strength_tablet=”1px” header_text_shadow_horizontal_length=”header_text_shadow_style,%91object Object%93″ header_text_shadow_horizontal_length_tablet=”0px” header_text_shadow_vertical_length=”header_text_shadow_style,%91object Object%93″ header_text_shadow_vertical_length_tablet=”0px” header_text_shadow_blur_strength=”header_text_shadow_style,%91object Object%93″ header_text_shadow_blur_strength_tablet=”1px” header_2_text_shadow_horizontal_length=”header_2_text_shadow_style,%91object Object%93″ header_2_text_shadow_horizontal_length_tablet=”0px” header_2_text_shadow_vertical_length=”header_2_text_shadow_style,%91object Object%93″ header_2_text_shadow_vertical_length_tablet=”0px” header_2_text_shadow_blur_strength=”header_2_text_shadow_style,%91object Object%93″ header_2_text_shadow_blur_strength_tablet=”1px” header_3_text_shadow_horizontal_length=”header_3_text_shadow_style,%91object Object%93″ header_3_text_shadow_horizontal_length_tablet=”0px” header_3_text_shadow_vertical_length=”header_3_text_shadow_style,%91object Object%93″ header_3_text_shadow_vertical_length_tablet=”0px” header_3_text_shadow_blur_strength=”header_3_text_shadow_style,%91object Object%93″ header_3_text_shadow_blur_strength_tablet=”1px” header_4_text_shadow_horizontal_length=”header_4_text_shadow_style,%91object Object%93″ header_4_text_shadow_horizontal_length_tablet=”0px” header_4_text_shadow_vertical_length=”header_4_text_shadow_style,%91object Object%93″ header_4_text_shadow_vertical_length_tablet=”0px” header_4_text_shadow_blur_strength=”header_4_text_shadow_style,%91object Object%93″ header_4_text_shadow_blur_strength_tablet=”1px” header_5_text_shadow_horizontal_length=”header_5_text_shadow_style,%91object Object%93″ header_5_text_shadow_horizontal_length_tablet=”0px” header_5_text_shadow_vertical_length=”header_5_text_shadow_style,%91object Object%93″ header_5_text_shadow_vertical_length_tablet=”0px” header_5_text_shadow_blur_strength=”header_5_text_shadow_style,%91object Object%93″ header_5_text_shadow_blur_strength_tablet=”1px” header_6_text_shadow_horizontal_length=”header_6_text_shadow_style,%91object Object%93″ header_6_text_shadow_horizontal_length_tablet=”0px” header_6_text_shadow_vertical_length=”header_6_text_shadow_style,%91object Object%93″ header_6_text_shadow_vertical_length_tablet=”0px” header_6_text_shadow_blur_strength=”header_6_text_shadow_style,%91object Object%93″ header_6_text_shadow_blur_strength_tablet=”1px” box_shadow_horizontal_tablet=”0px” box_shadow_vertical_tablet=”0px” box_shadow_blur_tablet=”40px” box_shadow_spread_tablet=”0px” vertical_offset_tablet=”0″ horizontal_offset_tablet=”0″ z_index_tablet=”0″]<\/p>\n GS Bhat, Sourabh S Diwan<\/strong>, 2025<\/span>, “A review on laboratory experiments and numerical simulations mimicking convective cloud-like flows<\/a><\/span>” , S\u0101dhan\u0101 50 (2), 1-22<\/strong><\/p>\n Sourabh S Diwan, K R Sreenivasan<\/strong>, 2025<\/span>, “History of Indic sciences and philosophy as viewed by Professor Narasimha<\/a><\/span>” , S\u0101dhan\u0101 50 (1), 28<\/strong><\/p>\n