{"id":245,"date":"2016-02-28T12:41:14","date_gmt":"2016-02-28T17:41:14","guid":{"rendered":"https:\/\/engineering.jhu.edu\/gayme\/?page_id=245"},"modified":"2017-02-22T13:23:11","modified_gmt":"2017-02-22T18:23:11","slug":"networked-systems","status":"publish","type":"page","link":"https:\/\/engineering.jhu.edu\/gayme\/networked-systems\/","title":{"rendered":"Stability and Performance of Coupled Oscillator Networks"},"content":{"rendered":"<p>Many complex systems can be modeled as a network of interacting subsystems, each with simple dynamics. In this work we use oscillator networks as a model of power grids and vehicular platoons. By applying tools from control theory to this modeling framework we investigate the effect of network structure on the synchronization performance of such systems. We show that for a large class of performance measures, the performance is determined by effective resistances in the underlying graphs. These results show the strong connection between the synchronization performance of oscillator networks\u00a0and circuit theory. Applications include evaluating the transient resistive losses due to maintaining synchrony in power grids as well as quantifying the coherence of vehicular platoons with different control laws and communication structures.<\/p>\n<p>Nodes<\/p>\n<p>We can use oscillator networks to evaluate a network\u2019s synchronization performance.\u00a0 Synchrony exists when all subsystems, or agents in a system, reach a mutual goal.\u00a0 To improve the performance of a network, we can tune the dynamics at particular nodes, as shown in the diagram below.<\/p>\n<p><a href=\"https:\/\/engineering.jhu.edu\/gayme\/wp-content\/uploads\/2016\/02\/control1.png\"><img loading=\"lazy\" decoding=\"async\" class=\"alignnone size-full wp-image-353\" src=\"https:\/\/engineering.jhu.edu\/gayme\/wp-content\/uploads\/2016\/02\/control1.png\" alt=\"\" width=\"1285\" height=\"321\" srcset=\"https:\/\/engineering.jhu.edu\/gayme\/wp-content\/uploads\/2016\/02\/control1.png 1285w, https:\/\/engineering.jhu.edu\/gayme\/wp-content\/uploads\/2016\/02\/control1-300x75.png 300w, https:\/\/engineering.jhu.edu\/gayme\/wp-content\/uploads\/2016\/02\/control1-768x192.png 768w, https:\/\/engineering.jhu.edu\/gayme\/wp-content\/uploads\/2016\/02\/control1-1024x256.png 1024w, https:\/\/engineering.jhu.edu\/gayme\/wp-content\/uploads\/2016\/02\/control1-250x62.png 250w, https:\/\/engineering.jhu.edu\/gayme\/wp-content\/uploads\/2016\/02\/control1-150x37.png 150w, https:\/\/engineering.jhu.edu\/gayme\/wp-content\/uploads\/2016\/02\/control1-1050x262.png 1050w\" sizes=\"auto, (max-width: 1285px) 100vw, 1285px\" \/><\/a><\/p>\n<p>&nbsp;<\/p>\n<p>Example Network: Vehicular Platoons<\/p>\n<p>In the case of vehicular platoons, synchronization would occur if the vehicles reach nominal spacing and velocity.\u00a0 Here, tuning the dynamics at particular nodes involves reducing communication in a vehicle platoon by tuning the leader\u2019s dynamics.<\/p>\n<p><a href=\"https:\/\/engineering.jhu.edu\/gayme\/wp-content\/uploads\/2016\/03\/platoon_combine.png\"><img loading=\"lazy\" decoding=\"async\" class=\"alignnone size-full wp-image-903\" src=\"https:\/\/engineering.jhu.edu\/gayme\/wp-content\/uploads\/2016\/03\/platoon_combine.png\" alt=\"\" width=\"584\" height=\"294\" srcset=\"https:\/\/engineering.jhu.edu\/gayme\/wp-content\/uploads\/2016\/03\/platoon_combine.png 584w, https:\/\/engineering.jhu.edu\/gayme\/wp-content\/uploads\/2016\/03\/platoon_combine-300x151.png 300w\" sizes=\"auto, (max-width: 584px) 100vw, 584px\" \/><\/a><\/p>\n<p>&nbsp;<\/p>\n<p>Example Network: Power Grid<\/p>\n<p>In the case of power grids, synchronization is reached when all generator phases reach nominal conditions with constant angular velocities.\u00a0 The cost associated with resynchronization, then, would be the transient losses of energy in a power grid.\u00a0 We can improve the performance by tuning a droop-controlled inverter and therefore reduce the resistive losses due to maintaining synchrony.\u00a0 The droop-control approximates the average power versus frequency properties of a synchronous generator, but has different dynamics.<\/p>\n<div id=\"attachment_309\" style=\"width: 943px\" class=\"wp-caption alignnone\"><a href=\"https:\/\/engineering.jhu.edu\/gayme\/wp-content\/uploads\/2016\/02\/power_grid_flat-e1473368183747.jpg\"><img loading=\"lazy\" decoding=\"async\" aria-describedby=\"caption-attachment-309\" class=\"size-full wp-image-309\" src=\"https:\/\/engineering.jhu.edu\/gayme\/wp-content\/uploads\/2016\/02\/power_grid_flat-e1473368183747.jpg\" alt=\"\" width=\"933\" height=\"255\" \/><\/a><p id=\"caption-attachment-309\" class=\"wp-caption-text\">Power Grid<\/p><\/div>\n","protected":false},"excerpt":{"rendered":"<p>Many complex systems can be modeled as a network of interacting subsystems, each with simple dynamics. In this work we use oscillator networks as a model of power grids and vehicular platoons. By applying tools from control theory to this modeling framework we investigate the effect of network structure on the synchronization performance of such [&hellip;]<\/p>\n","protected":false},"author":168,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"_exactmetrics_skip_tracking":false,"_exactmetrics_sitenote_active":false,"_exactmetrics_sitenote_note":"","_exactmetrics_sitenote_category":0,"footnotes":""},"class_list":["post-245","page","type-page","status-publish","hentry"],"yoast_head":"<!-- This site is optimized with the Yoast SEO plugin v27.8 - https:\/\/yoast.com\/product\/yoast-seo-wordpress\/ -->\n<title>Stability and Performance of Coupled Oscillator Networks - Dennice F. 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By applying tools from control theory to this modeling framework we investigate the effect of network structure on the synchronization performance of such [&hellip;]\" \/>\n<meta property=\"og:url\" content=\"https:\/\/engineering.jhu.edu\/gayme\/networked-systems\/\" \/>\n<meta property=\"og:site_name\" content=\"Dennice F. 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