- published: 02 Mar 2010
- views: 13306
'+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; })); }); -->
The speed of light in vacuum, commonly denoted c, is a universal physical constant important in many areas of physics. Its precise value is 7008299792458000000♠299792458 metres per second (approximately 7008300000000000000♠3.00×108 m/s), since the length of the metre is defined from this constant and the international standard for time. According to special relativity, c is the maximum speed at which all matter and information in the universe can travel. It is the speed at which all massless particles and changes of the associated fields (including electromagnetic radiation such as light and gravitational waves) travel in vacuum. Such particles and waves travel at c regardless of the motion of the source or the inertial reference frame of the observer. In the theory of relativity, c interrelates space and time, and also appears in the famous equation of mass–energy equivalence E = mc2.
The speed at which light propagates through transparent materials, such as glass or air, is less than c; similarly, the speed of radio waves in wire cables is slower than c. The ratio between c and the speed v at which light travels in a material is called the refractive index n of the material (n = c / v). For example, for visible light the refractive index of glass is typically around 1.5, meaning that light in glass travels at c / 1.5 ≈ 7008200000000000000♠200000 km/s; the refractive index of air for visible light is about 1.0003, so the speed of light in air is about 7008299700000000000♠299700 km/s (about 7004900000000000000♠90 km/s slower than c).
In Conway's Game of Life (and related cellular automata), the speed of light is a propagation rate across the grid of exactly one step (either horizontally, vertically or diagonally) per generation. In a single generation, a cell can only influence its nearest neighbours, and so the speed of light (by analogy with the speed of light in physics) is the maximum rate at which information can propagate. It is therefore an upper bound to the speed at which any pattern can move.
As in physics, the speed of light is represented with the letter . This in turn is used as a reference for describing the average propagation speed of any given type of spaceship. For example, a glider is said to have a speed of , as it takes four generations for a given state to be translated by one cell. Similarly, the "lightweight spaceship" is said to have a speed of , as it takes four generations for a given state to be translated by two cells.
While is an absolute upper bound to propagation speed, the maximum speed of a spaceship in Conway's Game of Life is in fact . This is because it is impossible to build a spaceship that can move every generation. (This is not true, though, for cellular automata in general; for instance many light-speed spaceships exist in Seeds.) It is, however, possible for objects to travel at the speed of light if they move through a medium other than empty space. Such media include trails of hives, and alternating stripes of live and dead cells.
The speed of light is a physical constant, the rate at which light travels in a vacuum.
Speed of Light may also refer to:
Cressida (/ˈkrɛsᵻdə/; also Criseida, Cresseid or Criseyde) is a character who appears in many Medieval and Renaissance retellings of the story of the Trojan War. She is a Trojan woman, the daughter of Calchas, a Greek seer. She falls in love with Troilus, the youngest son of King Priam, and pledges everlasting love, but when she is sent to the Greeks as part of a hostage exchange, she forms a liaison with the Greek warrior Diomedes. In later culture she becomes an archetype of a faithless lover.
The character's name is derived from that of Chryseis, a character who appears in the Iliad but has no connection with Troilus, Diomedes or Calchas. Indeed, the story of Troilus and Cressida does not appear in any Greek legends but was invented by the twelfth century French poet Benoît de Sainte-Maure in the Roman de Troie. The woman in the love triangle is here called not Cressida but Briseida, a name derived from that of Briseis, a different character in the Iliad, who again is neither related to Calchas nor involved in any love affairs with Troilus or Diomedes. Initially, after the Roman appeared, other authors who refer to the story, for example, Azalais d'Altier in her poem Tanz salutz e tantas amors and Guido delle Colonne in his Historia destructionis Troiae, continue to use names derived from that of Briseis.
The following is a list of characters in The Hunger Games trilogy, a series of young adult science fiction novels by Suzanne Collins that were later adapted into a series of four feature films.
Cressida (/ˈkrɛsᵻdə/ KRES-i-də, Greek: Χρησίδα) is a character in Medieval and Renaissance literature. Cressida may also refer to:
As a given name:
Download here: http://tinyurl.com/uniteddestination2010 As the lights fade and the volume rises, the dance scene awakes. They gather in big groups to share their belief, no matter what nationality or ethnicity. Theyre all here for the same reason. Music is the unifying factor, an unspoken language common to all. Dash Berlin welcomes you to the nocturnal society. Dash Berlin:We are all connected by sound. The place where we celebrate tonight, is our United Destination 2010. The Dash Berlin sound has reached deep into the heart of the dance scene and far across the EDM places of this world. It all started three years ago, when first single Till The Sky Falls Down turned the heads and popped the ears. Today, front man Jeffrey Suttorius is the proud owner of Aropa Records and looks back ...
tyDi feat. Sarah Howells - When I Go (Arnej Remix) ★★★【MUSIC VIDEO ToJ edit】★★★ Buy here: http://www.beatport.com/#/release/when-i-go-e-p/1024180 ASOT 596 - Armin van Buuren Playlist for A State of Trance episode 596. 17-01-2013. 1.Andy Moor & Betsie LarkinLove Again (Andrew Rayel Remix) [AVA Recordings] 2.Denis Kenzo feat. Sveta B.Lullaby Lonely (Progressive mix) [Infrasonic Progressive] 3.AudienWayfarer [Anjunabeats] 4.Vadim SparkLost Angeles (Club Mix) [Vendace] 5.Kyau & AlbertAll Your Colours [Euphonic] 6.Steve Brian & CressidaCasablanca [Tooltrance] 7.EximindsMainbeat [Garuda] 8.Antillas & DankannSynapse (Club Mix) [Soundpiercing] 9.Dennis Sheperd & Cold Blue feat. Ana CriadoFallen Angel (Lange Remix) [High Contrast] 10.FUTURE FAVORITE: Armin van Buuren & Markus SchulzThe Expeditio...
Robimon feat. Tiff Lacey - Goodbye (Cressida Remix) (2008). Amazing!
Download on iTunes: http://bit.ly/Arena_IT Listen on Spotify: http://bit.ly/Arena_SF Download on Beatport: http://bit.ly/ArenaBP Check this item on ArmadaMusic.com: http://bit.ly/Arena_Webs Follow us: http://www.facebook.com/armadamusic https://www.facebook.com/perfectorecords They've remixed for us twice recently - on both Michael S. and Kenneth Thomas's current singles on Perfecto. So getting an EP from these hugely talented producers that all in the Perfecto office love seemed a natural progression. Did we mention... We all love Swab & Joey Mova. It's vocal, it's instrumental, it's progressive, it's techno, it's melodic, it's blissful, it's dark, it's light, it's big... oh so very big. Come into the Arena - Swab & Joey Mova are on. Tracks: Lux In Tenebris (Vocal Mix) (08:03) Lux...
Signed CD: http://bit.ly/Remixed-CD iTunes: http://bit.ly/Remixed-iT Beatport: http://bit.ly/Remixed-BP Amazon: http://amzn.to/Remixed-AZ Juno Download: http://bit.ly/Remixed-JD DJ Download: http://bit.ly/Remixed-DJ Track It Down: http://bit.ly/Remixed-TID Lange Remixed - Released 17th October 2011 Lange, the UK's number 1 trance producer, responsible for numerous chart hits and club anthems, revisits the best of his label with a double remixed album out on Lange Recordings on October 17th. The album features some of the best remixes from the catalogue alongside brand new takes on Lange classics that feature on the label. Lange has strived over the past 7 years to create a label that focuses on quality rather than quantity with tracks that reflect his own fusion of melody and...
ATB & Mirco De Govia Vital Rain Vexilium Mix
Ron Hagen & Pascal M - Riddles In The Sand (Omnia Remix) vs Markus Schoessow , Andy Duguid & Emma Hewitt - Light (Omnia mashup) Artist(s) .........:: Armin van Buuren Title .............:: A State of Trance Episode 443 Genre .............:: Trance Source ............:: Radio Quality ...........:: 256 kbps / 44,1 kHz Duration ..........:: 02:01:01 Release Date ......:: 11-02-2010 Support ...........:: www.di.fm Tracklist .........:: 1. Ron Hagen & Pascal M - Riddles In The Sand (Omnia Remix) vs Markus Schoessow , Andy Duguid & Emma Hewitt - Light (Omnia mashup) 2. Deep Night - Escape 3. Beat Service feat. Emma Lock - Hiding To Nothing 4. Brave - The Healer 5. Steve Brian - La Gomera (Cressida Remix) (Future Favourite) 6. Rex Mundi - Candy Land 7. Ali Wilson - Pando...
out NOW! Beatport : http://bit.ly/ificould-bp TrackItDown : http://bit.ly/ificould-trackitdown iTunes : http://bit.ly/ificould-itunes Juno Download : http://bit.ly/ificould-juno 7Digital : http://bit.ly/ificould-7digital Dance-Tunes : http://bit.ly/ificould-dt (As played by Armin van Buuren on A State Of Trance 477) Also check out: Album Mix - http://youtu.be/hmggRcGMbJs Club Mix - http://youtu.be/X9hJOi9MdSU 2001 Returning Mix - http://youtu.be/2j75qyyUngw 2001 Returning Dub - http://youtu.be/0nELH23AQJ4 Dan Stone Dub Mix - http://youtu.be/-BOBs7AXMIE Susana & Bart Claessen - If I Could (Dan Stone remix) :: Armada release: December 2010 -------------------- http://www.bartclaessen.com http://www.twitter.com/bartclaessen http://www.facebook.com/bartclaessen
The speed of light in vacuum, commonly denoted c, is a universal physical constant important in many areas of physics. Its precise value is 7008299792458000000♠299792458 metres per second (approximately 7008300000000000000♠3.00×108 m/s), since the length of the metre is defined from this constant and the international standard for time. According to special relativity, c is the maximum speed at which all matter and information in the universe can travel. It is the speed at which all massless particles and changes of the associated fields (including electromagnetic radiation such as light and gravitational waves) travel in vacuum. Such particles and waves travel at c regardless of the motion of the source or the inertial reference frame of the observer. In the theory of relativity, c interrelates space and time, and also appears in the famous equation of mass–energy equivalence E = mc2.
The speed at which light propagates through transparent materials, such as glass or air, is less than c; similarly, the speed of radio waves in wire cables is slower than c. The ratio between c and the speed v at which light travels in a material is called the refractive index n of the material (n = c / v). For example, for visible light the refractive index of glass is typically around 1.5, meaning that light in glass travels at c / 1.5 ≈ 7008200000000000000♠200000 km/s; the refractive index of air for visible light is about 1.0003, so the speed of light in air is about 7008299700000000000♠299700 km/s (about 7004900000000000000♠90 km/s slower than c).
3 a.m and you're tossing in your bed
Thoughts are turning in your head
You're hanging on, but how much longer
Why do empty things you pour your soul into
Never fill that void in you, makes you wonder
There are shadows hanging over you
I know you wish that you could see beyond
But it's always darkest before the dawn
Love at the speed of light comes on the darkest night
And it only takes a moment to change a life
All of us need is love come see the wonder of
The miracle that happens when we believe
Love at the speed of light comes on the darkest night
It only takes a moment to make us right
We can believe in love
We can be free at the speed of light
I've heard it said the peace of mind that you desire
Is in the power that you acquire
You're moving up, but how much longer
What's the matter if you gain a wealth of gold
But in the process you lose your soul, you have to wonder
There is darkness surrounding you
I hear you pray that you could see the sun
And that's the moment your freedom comes
Love at the speed of light comes on the darkest night
And it only takes a moment to change a life
All of us need is love come see the wonder of
The miracle that happens when we believe
Love at the speed of light comes on the darkest night
It only takes a moment to make us right
We can believe in love
We can be free at the speed of light
Break away, leave the cold night
Steal away from the shadows
Break away, leave the old life
Dance away from the dark
Love at the speed of light comes on the darkest night
And it only takes a moment to change a life
All of us need is love come see the wonder of
The miracle that happens when we believe
Love at the speed of light comes on the darkest night
And it only takes a moment to make us right
We can believe in love
We can be free at the speed of light
Love at the speed of light comes on the darkest night
Only takes a moment to change a life
All of us need is love come see the wonder of
The miracle that happens when we believe
Love at the speed of light comes on the darkest night
And it only takes a moment to make us right
We can believe in love