'+pages+''); $('.stream > div:odd').addClass('bgr_color'); updateHeight('#history'); }); window.activateTabArea = ensure(function(tab, areas){ var parsed = false; var parts = (areas || '').split('/'); window.fsonload = $.inArray('fs', parts) >= 0; if(fsonload){ parts.splice(parts.indexOf('fs'), 1); } var replayMode = false; if($.inArray('replay', parts)>=0){ replayMode = 'replay'; } var noSoundMode = false; if($.inArray('nosound', parts)>=0){ noSoundMode = 'nosound'; } if($.inArray('ns', parts)>=0){ noSoundMode = 'ns'; } var previewMode = null; if($.inArray('p', parts)>=0){ previewMode = 'p'; } if($.inArray('preview', parts)>=0){ previewMode = 'preview'; } if($.inArray('repeat', parts)>=0){ replayMode = 'repeat'; } if($.inArray('r', parts)>=0 || $.inArray('ro', parts)>=0){ replayMode = 'r'; } if(replayMode){ parts.splice(parts.indexOf(replayMode), 1); } if(noSoundMode){ parts.splice(parts.indexOf(noSoundMode), 1); } if(previewMode){ parts.splice(parts.indexOf(previewMode), 1); } if(previewMode){ if(!parts.length){ parts = ['1-14', '999:59']; } } var area = parts[0]; if(tab == 'history' && false){ var page = parseInt(area || '1') || 1; $.ajax({ url: 'https://login.wn.com/recent/json/?pp='+history_pp+'&skip='+history_pp*(page-1), dataType: 'jsonp', success: function(response){ $ensure(function(){ renderHistory(response, page); }); } }); return true; } if(tab == 'global_history' && false){ var page = parseInt(area || '1') || 1; globalHistory.fetchStream(page, '', function(){ updateHeight('#global_history'); }); return true; } if(tab == 'my_playlists' && false){ var page = parseInt(area || '1') || 1; myPlaylists.fetchStream(page, '', function(){ updateHeight('#my_playlists'); }); return true; } if(tab == 'my_videos' && false){ var page = parseInt(area || '1') || 1; myVideos.fetchStream(page, '', function(){ updateHeight('#my_videos'); }); return true; } if(tab == 'related_sites' && areas && matchPosition(areas)){ var seconds = parsePosition(areas); scrollRelated(seconds); return false; } if(matchPosition(area) || matchAction(area)){ parts.unshift('1'); area = parts[0]; } if(tab == 'expand' && area && area.match(/\d+/)) { var num = parseInt(area); if(num < 100){ //FIX ME. Load news page with ajax here } else if(num > 1900){ //FIX ME. Load timeline page with ajax here } } else if(tab.match(/^playlist\d+$/)){ var playerId = parseInt(tab.substring(8)); var vp = videoplayers[playerId]; window.descriptionsholder = $('.descriptionsplace'); if(!vp) return; // why? no player? if(replayMode){ $('.replaycurrent'+playerId).attr('checked', true); vp.setReplayCurrent(true); } var playQueue = []; window.playQueue = playQueue; var playQueuePosition = 0; var playShouldStart = null; var playShouldStop = null; var parseList = function(x){ var items = x.split(/;|,/g); var results = []; for (i in items){ try{ var action = parseAction(vp, items[i]); if(!action.video){ if(window.console && console.log) console.log("Warning: No video for queued entry: " + items[i]); }else{ results.push(action); } }catch(e){ if(window.console && console.log) console.log("Warning: Can''t parse queue entry: " + items[i]); } } return results; }; var scrollToPlaylistPosition = function(vp){ var ppos = vp.getPlaylistPosition(); var el = vp.playlistContainer.find('>li').eq(ppos); var par = el.closest('.playlist_scrollarea'); par.scrollTop(el.offset().top-par.height()/2); } var updateVolumeState = function(){ if(noSoundMode){ if(noSoundMode == 'turn-on'){ clog("Sound is on, vsid="+vp.vsid); vp.setVolumeUnMute(); noSoundMode = false; }else{ clog("Sound is off, vsid="+vp.vsid); vp.setVolumeMute(); noSoundMode = 'turn-on'; } } } var playQueueUpdate = function(){ var playPosition = playQueue[playQueuePosition]; vp.playFromPlaylist(playPosition.video); scrollToPlaylistPosition(vp); playShouldStart = playPosition.start; playShouldStop = playPosition.stop; }; var playQueueAdvancePosition = function(){ clog("Advancing play position..."); playQueuePosition ++; while(playQueuePosition < playQueue.length && !playQueue[playQueuePosition].video){ playQueuePosition ++; } if(playQueuePosition < playQueue.length){ playQueueUpdate(); }else if(vp.getReplayCurrent()){ playQueuePosition = 0; playQueueUpdate(); vp.seekTo(playShouldStart); vp.playVideo(); }else{ vp.pauseVideo(); playShouldStop = null; playShouldStart = null; } }; function loadMoreVideos(playerId, vp, start, finish, callback){ var playlistInfo = playlists[playerId-1]; if(playlistInfo.loading >= finish) return; playlistInfo.loading = finish; $.ajax({ url: '/api/upge/cheetah-photo-search/query_videos2', dataType: 'json', data: { query: playlistInfo.query, orderby: playlistInfo.orderby, start: start, count: finish-start }, success: function(response){ var pl = vp.getPlaylist().slice(0); pl.push.apply(pl, response); vp.setPlaylist(pl); callback(); } }); } if(parts.length == 1 && matchDash(parts[0])){ var pl = vp.getActualPlaylist(); var vids = parseDash(parts[0]); parts = []; for(var i = 0; i < vids.length; i++){ playQueue.push({ 'video': pl[vids[i]-1], 'start': 0, 'stop': null }) } if(vids.length){ if(vids[vids.length-1]-1>=pl.length){ loadMoreVideos(playerId, vp, pl.length, vids[vids.length-1], function(){ if(fsonload){ activateTabArea(tab, parts[0]+'/fs'); }else{ activateTabArea(tab, parts[0]); } var pls = vp.getPlaylist(); vp.playFromPlaylist(pls[pls.length-1]); vp.playVideo(); scrollToPlaylistPosition(vp); }); return true; } } if(playQueue){ playQueueUpdate(); vp.playVideo(); parsed = true; playShouldStart = 0; } } if(previewMode){ var vids = []; var dur = 0; var pl = vp.getActualPlaylist(); area = parts[0]; if(parts.length == 1 && matchPosition(parts[0])){ vids = parseDash('1-'+pl.length); dur = parsePosition(parts[0]); parts = []; }else if(parts.length == 1 && matchDash(parts[0])){ vids = parseDash(parts[0]); dur = parsePosition("999:59"); parts = []; } if(parts.length == 2 && matchDash(parts[0]) && matchPosition(parts[1])){ vids = parseDash(parts[0]); dur = parsePosition(parts[1]); parts = []; } for(var i = 0; i < vids.length; i++){ playQueue.push({ 'video': pl[vids[i]-1], 'start': 0, 'stop': dur }) } if(playQueue){ playQueueUpdate(); vp.playVideo(); parsed = true; } } if(parts.length>1){ for(var i = 0; i < parts.length; i++){ var sel = findMatchingVideo(vp, parts[i]); if(sel){ playQueue.push({ 'video': sel, 'start': 0, 'stop': null }) } } if(playQueue){ playQueueUpdate(); vp.playVideo(); parsed = true; } }else if(area){ var sel = findMatchingVideo(vp, area); if(sel){ vp.playFromPlaylist(sel); playShouldStart = 0; parsed = true; } } if(fsonload || replayMode){ playShouldStart = 0; } if(document.location.search.match('at=|queue=')){ var opts = document.location.search.replace(/^\?/,'').split(/&/g); for(var o in opts){ if(opts[o].match(/^at=(\d+:)?(\d+:)?\d+$/)){ playShouldStart = parsePosition(opts[o].substr(3)) } if(opts[o].match(/^queue=/)){ playQueue = parseList(opts[o].substr(6)); if(playQueue){ playQueuePosition = 0; playQueueUpdate(); } } } } if(matchPosition(parts[1])){ playShouldStart = parsePosition(parts[1]); parsed = true; } if(matchAction(parts[1])){ var action = parseAction(vp, area+'/'+parts[1]); playShouldStart = action.start; playShouldStop = action.stop; parsed = true; } if(playShouldStart !== null && !playQueue.length){ playQueue.push({ video: vp.getCurrentVideo(), start: playShouldStart, stop: playShouldStop }); } if(playShouldStart != null){ setInterval(function(){ if(playShouldStop && vp.currentPlayer && vp.currentPlayer.getCurrentTime() > playShouldStop){ playShouldStop = null; if(vp.getCurrentVideo() == playQueue[playQueuePosition].video){ playQueueAdvancePosition(); }else{ playShouldStart = null; } } }, 500); vp.playerContainer.bind('videoplayer.player.statechange', function(e, state){ if(state == 'ended'){ // advance to the next video playQueueAdvancePosition(); } }); vp.playerContainer.bind('videoplayer.player.readychange', function(e, state){ if(state){ updateVolumeState(); if(playShouldStart !== null){ vp.seekTo(playShouldStart); playShouldStart = null; }else{ playShouldStop = null; // someone started other video, stop playing from playQueue } } if(fsonload) { triggerFullscreen(playerId); fsonload = false; } }); } } else if(tab.match(/^wiki\d+$/)){ if(firstTimeActivate){ load_wiki($('#'+tab), function(){ if(area){ var areaNode = $('#'+area); if(areaNode.length>0){ $('html, body').scrollTop(areaNode.offset().top + 10); return true; } } }); } } return parsed; }) window.activateTab = ensure(function(tab, area){ window.activeArea = null; if(tab == 'import_videos'){ if(area){ import_videos(area); }else{ start_import(); } return true; } if(tab == 'chat'){ update_chat_position($('.chat').eq(0)); window.activeArea = 'chat'; jQuery('.tabtrigger').offscreentabs('activateTab', 'chat'); return true; } if(tab in rev_names){ tab = rev_names[tab]; } if(tab.match(':')){ return false; } var sup = $('ul li a[id=#'+tab+']'); if(sup && sup.length>0){ window.activeArea = area; sup.first().click(); if(!window.activateTabArea(tab, area)){ window.activeArea = null; } window.activeArea = null; return true; }else{ var have_tabs = $('#playlist_menu li').length; if(tab.match(/^playlists?\d+$/)){ var to_add = +tab.substring(8).replace(/^s/,'')-have_tabs; if(to_add>0 && have_tabs){ add_more_videos(to_add); return true; } } } return false; }); window.currentPath = ensure(function(){ return window.lastHistory.replace(basepath, '').split('?')[0]; }); window.main_tab = window.main_tab || 'videos'; window.addHistory = ensure(function(path){ if(window.console && console.log) console.log("Adding to history: "+path); if(window.history && history.replaceState && document.location.hostname.match(/^(youtube\.)?(\w{2,3}\.)?wn\.com$/)){ if(path == main_tab || path == main_tab+'/' || path == '' || path == '/') { path = basepath; } else if( path.match('^'+main_tab+'/') ){ path = basepath + '/' + path.replace(main_tab+'/', '').replace('--','/'); } else { path = basepath + '/' + path.replace('--','/'); } if(document.location.search){ path += document.location.search; } if(window.lastHistory) { history.pushState(null, null, path); } else if(window.lastHistory != path){ history.replaceState(null, null, path); window.lastHistory = path; } } else{ path = path.replace('--','/'); if(path == main_tab || path == main_tab+'/' || path == '' || path == '/') { path = ''; } if(window.lastHistory != '/'+path){ window.location.hash = path? '/'+path : ''; window.lastHistory = '/'+path; } } }); $('.tabtrigger li a').live('click', ensure(function() { var tab = $(this).attr('id'); if(tab.substring(0,1) == '#'){ var name = tab.substring(1); if(name in menu_names){ name = menu_names[name][0]; } realTab = rev_names[name]; $('#'+realTab).show(); if(window.console && console.log) console.log("Triggering tab: "+name+(window.activeArea?" activeArea="+window.activeArea:'')); var path = name; if(window.activeArea){ path = path + '/' + window.activeArea; } if(tab.match(/#playlist\d+/) || tab.match(/#details\d+/)){ $('.multiple-playlists').show(); $('.related_playlist').show(); $('.longest_videos_playlist').show(); }else { $('.multiple-playlists').hide(); $('.related_playlist').hide(); $('.longest_videos_playlist').hide(); } // start the related script only when the tab is on screen showing if (tab.match(/related_sites/)) { if (mc) { mc.startCredits(); } } window.activeTab = realTab; addHistory(path); setTimeout(ensure(function(){ if(tab.match(/language--/)){ $('.tabtrigger').offscreentabs('activateTab', 'language'); } if(tab.match(/weather/)) { $('.tabtrigger').offscreentabs('activateTab', 'weather'); loadContinent(); } updateMenus(tab); updateHeight(); }), 10); } return false; })); }); -->

' }else{ weather_info += '
'+tempC+' °C
' } weather_info += '
  • Pressure: '+weather_data.main.pressure+' hPa
  • ' if (weather_data.main.humidity) { weather_info += '
  • Humidity: '+weather_data.main.humidity+' %
  • '; } if (clouds) { weather_info += '
  • Clounds: '+clouds.all+'%
  • ' } if (weather) { weather_info += '
  • '+weather.description+'
  • ' } weather_info += '
' } } global_geo_obj.html(weather_info); var global_geo = jQuery('#forecast'); get_forecast_details(city, 4, global_geo, country); }) }); }); function forecast_status(msg) { jQuery('#forecast-header').html(msg); } function get_forecast_details(city, days_count, global_geo, country) { global_geo.html('Loading forecast ...'); jQuery.ajax({ data: { city: city, report: 'daily' }, dataType: 'jsonp', url: 'https://upge.wn.com/api/upge/cheetah-photo-search/weather_forecast_4days', success: function(data) { if(!data) { text = ('weater data temporarily not available'); } // loop through the list of weather info weather_info = ''; var weather_day_loop = 0; jQuery.each(data.list, function(idx, value) { if (idx < 1) { return; } if (weather_day_loop >= days_count) { return false; } weather = value.weather.shift() clouds = value.clouds d = new Date(value.dt*1000) t = d.getMonth()+1 + '-' + d.getDate() + '-' + d.getFullYear() moment.lang('en', { calendar : { lastDay : '[Yesterday]', sameDay : '[Today]', nextDay : '[Tomorrow]', lastWeek : '[last] dddd', nextWeek : 'dddd', sameElse : 'L' } }); mobj = moment(value.dt*1000) // skip today if (t == today) { return; } tempC = parseInt(parseFloat(value.temp.day)-273.15) tempF = parseInt(tempC*1.8+32) today = t; weather_day_loop += 1; weather_info += '
'+mobj.calendar()+'
'; weather_info += '
' weather_info += '
' if (country == 'United States'){ weather_info += '
'+tempF+' °F
' }else{ weather_info += '
'+tempC+' °C
' } weather_info += '
  • '+value.pressure+' hPa
  • ' if (value.humidity) { weather_info += '
  • Humidity: '+value.humidity+' %
  • '; } if (clouds) { weather_info += '
  • Clouds: '+clouds+'%
  • ' } if (weather) { weather_info += '
  • ' +weather.description+'
  • ' } weather_info += '
' }); global_geo.html(weather_info); } }); } //-->
'); } else { var query = elem.find('.keywords').html(); $.ajax({ context: elem, url: 'https://wn.com/api/upge/cheetah-search-adv/video', cache: true, data: { 'query': query }, dataType: 'jsonp', success: function(text) { if (text.length > 0) { video_id = text[0].id; elem.find('.player').html(''); } } }); } } var stopAllYouTubeVideos = function() { var iframes = document.querySelectorAll('iframe'); Array.prototype.forEach.call(iframes, function(iframe) { iframe.contentWindow.postMessage(JSON.stringify({ event: 'command', func: 'pauseVideo' }), '*'); }); } jQuery(function() { jQuery(".playVideo").live("click", function() { if(!$(this).hasClass("played")){ stopAllYouTubeVideos(); var elem = $(this); setTimeout(function(){ mouseOverMe(elem); }, 1000); } }); jQuery(".description_box .expandContent").live("click", function() { elem = $(this).parent().parent().parent().find('.descContent'); if(elem.height() > 51) { elem.css('height', '44px'); $(this).html('Show More '); }else{ elem.css('height', 'auto'); $(this).html('Hide '); } }); jQuery('.interview-play-off').click(function() { $(".interview-play-off").hide(); $(".interview-play").show(); $(".videoplayer-control-pause").click(); }); jQuery(".video-desc .show_author_videos").live("click", function() { query = $(this).attr('title'); container = $(this).parent().parent().parent().find('.video-author-thumbs'); $(this).parent().parent().parent().find('.video-author-thumbs').css('height', '220px'); jQuery.ajax({ url: '/api/upge/cheetah-photo-search/videoresults', data: {'query': query}, success: function(text) { if(!text) { text = i18n("No results"); } container.html(jQuery(text)); } }); }); }); // -->

Latest News for: brenna, poland

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Section III softball stats leaders (through May 9)

The Post-Standard 10 May 2024
Updated. May. 10, 2024, 9.00 a.m ... Maddison Haver Poland 28 ... Bradie Jones Poland 17 ... Bradie Jones Poland 4 ... Brenna Hogan Cortland 4 ... Hailey Haver Poland 18 ... Maddison Haver Poland 18 ... Emma Kraszewski Poland 14 ... McKenzie Parow Poland 13 ... Brenna Hogan Cortland 114.
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Section III softball stats leaders (through May 2)

The Post-Standard 03 May 2024
Maddison Haver Poland 26 ... Brenna Hogan Cortland 19 ... Hailey Haver Poland 18 ... Emma Kraszewski Poland 17 ... Bradie Jones Poland 16 ... Bradie Jones Poland 17 ... Emma Tabor Poland 14 ... Emma Kraszewski Poland 14. Brenna Hogan Cortland 14 ... McKenzie Parow Poland 12.
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Section III girls basketball rebounding leaders, ranked by year in school (through Jan. 24)

The Post-Standard 25 Jan 2024
Updated. Jan. 25, 2024, 11.30 a.m. East Syracuse Minoa’s Aniyah Jones is among the leading Section III juniors in rebounds per game.Scott Schild . [email protected] ... By Pat Spadafore ... Maddison Haver Poland 12 82 6.8 ... Brenna Seamon Cooperstown 15 97 6.5.
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Section III girls basketball rebounding leaders, ranked by year in school (through Jan. 10)

The Post-Standard 11 Jan 2024
Updated. Jan. 11, 2024, 11.30 a.m ... Scott Schild . [email protected] Schild . [email protected]. Subscribers can gift articles to anyone ... 10 ... Lily Martin Poland 7 47 6.7. Maddison Haver Poland 7 47 6.7 ... Brenna Seamon Cooperstown 12 79 6.6 ... Disclaimer.
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Section III girls basketball steals leaders, ranked by year in school (through Jan. 10)

The Post-Standard 11 Jan 2024
Updated. Jan. 11, 2024, 12.00 p.m. Auburn's Peyton Maneri, here against East Syracuse Minoa last week, is among the Section III senior leaders in steals. Scott Schild ... 10 ... Maddison Haver Poland 7 21 3 ... Brenna Seamon Cooperstown 12 33 2.8 ... Ella St ... ....
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Top returning Section III girls basketball leaders, ranked by 2022-23 assists

The Post-Standard 07 Nov 2023
Updated. Nov. 07, 2023, 11.30 a.m. Auburn's Peyton Maneri is among the leading returning senior assists leaders. Marilu Lopez Fretts. By Pat Spadafore ... Player School AST ... Maddison Haver Poland 34. Brenna Seamon Cooperstown 32 ... Lily Martin Poland 30 ... ....
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Section III girls soccer stats playoff leaders (through Oct. 21)

The Post-Standard 23 Oct 2023
Updated. Oct. 23, 2023, 9.30 a.m ... 21 ... Lily Martin Poland 3 2 8 ... Emily Satterlee Poland 3 0 6 ... Emily Satterlee Poland 3 ... Lily Martin Poland 3 ... Lily Martin Poland 2. Maddison Haver Poland 2 ... Zyanna Irving-Summers Poland 10. Brenna Seamon Cooperstown 10 ... ....
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Section III CSC softball stats leaders through May 11

The Post-Standard 12 May 2023
Shelbi Hagues Poland 33 16 ... Brenna Seamon Cooperstown 29 13 ... Shelbi Hagues Poland 33 13 ... Maddison Haver Poland 30 9 ... Brenna Seamon Cooperstown 29 5 ... Shelbi Hagues Poland 33 3 ... Maddison Haver Poland 30 1 ... Shelbi Hagues Poland 44 17.
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Section III softball stats leaders for Week 5

The Post-Standard 09 May 2023
Updated. May. 09, 2023, 9.30 a.m ... Marilu Lopez Fretts . Contributing photographerMarilu Lopez Fretts ... Shelbi Hagues Poland 33 16 ... Shelbi Hagues Poland 44 17 ... Brenna Hogan Cortland 77 29 ... Brenna Hogan Cortland 77 81. Shelbi Hagues Poland 44 81 ... Disclaimer ... ....
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Section III softball stats leaders for Week 2

The Post-Standard 18 Apr 2023
Updated. Apr. 18, 2023, 11.35 a.m ... She is pictured here with Colleen Jump ... NEW! ... Shelbi Hagues Poland 9 2 ... Maddison Haver Poland 9 1 ... Shelbi Hagues Poland 19 3 ... Brenna Hogan Cortland 28 9 ... Brenna Hogan Cortland 28 36. Shelbi Hagues Poland 19 36 ... Disclaimer ... ....
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Section III girls basketball sectional finals stats

The Post-Standard 06 Mar 2023
Logan Cookinham Poland 23 ... Brenna Seamon Cooperstown 11 ... Sydney Tabor Poland 11 ... Logan Cookinham Poland 14 ... Sydney Tabor Poland 9 ... Maddison Haver Poland 5 ... Brenna Seamon Cooperstown 2 ... Lily Martin Poland 2. Sydney Tabor Poland 2. Logan Cookinham Poland 2.
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Section III final regular-season girls soccer stats

The Post-Standard 17 Oct 2022
Updated. Oct ... NEW! ... Brenna Mast Beaver River 11 15 37 ... Lily Martin Poland 15 5 35 ... Logan Cookinham Poland 10 15 35 ... Lily Martin Poland 15 ... Brenna Mast Beaver River 11 ... Logan Cookinham Poland 15. Brenna Mast Beaver River 15 ... Brenna Seamon Cooperstown 113 ... ....
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Section III girls volleyball stats leaders (Week 4)

The Post-Standard 28 Sep 2022
Updated. Sep. 28, 2022, 10.30 a.m. Marcellus faced Skaneateles in girls volleyball earlier this month. Marilu Lopez Fretts . Contributing photographer Marilu Lopez Fretts. NEW!. By Pat Spadafore ... Lauren Poland Liverpool 5 ... Brenna Hogan Cortland 5 ... Disclaimer.
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Section III girls soccer stats leaders (Week 4)

The Post-Standard 26 Sep 2022
Updated. Sep. 26, 2022, 10.00 a.m ... She also scored her 150th career goal on Saturday ... NEW! ... Brenna Mast Beaver River 6 12 24 ... Lily Martin Poland 6 ... Brenna Mast Beaver River 6 ... Brenna Mast Beaver River 12 ... Logan Cookinham Poland 6 ... Brenna Seamon Cooperstown 48.
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Final Section III boys, girls basketball playoff scoring leaders

The Post-Standard 08 Mar 2022
Published. Mar. 08, 2022, 8.00 a.m. New Hartford’s Zach Philipkoski vs ... [email protected]. By Pat Spadafore . [email protected] ... Player School G Total PTS Total PTS Avg ... Logan Cookinham Poland 3 71 23.7. Brenna Mast Beaver River 1 22 22 ... Disclaimer.

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