{"product_id":"to-find-the-speed-of-sound-in-air-at-room-temperature-using-a-resonance-tube-by-two-resonance-positions","title":"TO FIND THE SPEED OF SOUND IN AIR AT ROOM TEMPERATURE USING A RESONANCE TUBE BY TWO RESONANCE POSITIONS.","description":"\u003cp\u003eAPPARATUS SUPPLIED WITH THIS EXPERIMENT\u003c\/p\u003e\n\u003col\u003e\n\u003cli\u003eRESONANCE TUBE APPARATUS (COMPLETE)\u003c\/li\u003e\n\u003cli\u003eTWO TUNING FORKS OF DIFFERENT FREQUENCY\u003c\/li\u003e\n\u003cli\u003eLAB MANUAL                                                                                                                       \u003cspan\u003eThe resonance tube experiment works on the principle of \u003c\/span\u003e\u003cmark class=\"HxTRcb\"\u003e\u003c!--qkimaf voqh4_1a\/HugV6--\u003e\u003c!--cqw1tb voqh4_1a\/HugV6--\u003e\u003cstrong class=\"rQesXe MPyX\"\u003eacoustic resonance\u003c!--TgQPHd|||[]--\u003e\u003c\/strong\u003e and the formation of \u003cstrong class=\"rQesXe MPyX\"\u003elongitudinal stationary (standing) waves\u003c!--TgQPHd|||[]--\u003e\u003c\/strong\u003e in a closed air column\u003c!--TgQPHd|||[]--\u003e\u003c\/mark\u003e. When a vibrating tuning fork is held over the open end, sound waves travel down and reflect off the water surface, creating a loud, amplified sound if the natural frequency of the air column matches the frequency of the fork.                                                                         \n\u003cdiv class=\"otQkpb\" role=\"heading\"\u003eCore Physics Concepts\u003c!--TgQPHd|||[]--\u003e\n\u003c\/div\u003e\n\u003cdiv class=\"\"\u003e\n\u003cspan class=\"iNqyIf\"\u003e\u003cstrong class=\"rQesXe MPyX\"\u003eResonance:\u003c!--TgQPHd|||[]--\u003e\u003c\/strong\u003e Maximum sound amplification happens when the forced frequency of the tuning fork equals the natural frequency of the enclosed air column.\u003c!--TgQPHd|||[]--\u003e\u003c\/span\u003e\u003c!--TgQPHd|||[]--\u003e\n\u003c\/div\u003e\n\u003cdiv class=\"\"\u003e\n\u003cspan class=\"iNqyIf\"\u003e\u003cstrong class=\"rQesXe MPyX\"\u003eNodes and Antinodes:\u003c!--TgQPHd|||[]--\u003e\u003c\/strong\u003e A displacement \u003cstrong class=\"rQesXe MPyX\"\u003enode\u003c!--TgQPHd|||[]--\u003e\u003c\/strong\u003e (zero particle motion) forms at the closed water surface, while a displacement \u003cstrong class=\"rQesXe MPyX\"\u003eantinode\u003c!--TgQPHd|||[]--\u003e\u003c\/strong\u003e (maximum particle motion) forms near the open top of the tube.\u003c!--TgQPHd|||[]--\u003e\u003c\/span\u003e\u003cspan\u003e \u003c\/span\u003e\u003c!--TgQPHd|||[]--\u003e\n\u003c\/div\u003e\n\u003cdiv class=\"\"\u003e\u003cspan class=\"iNqyIf\"\u003e\u003cstrong class=\"rQesXe MPyX\"\u003eWavelength Relation:\u003c!--TgQPHd|||[]--\u003e\u003c\/strong\u003e As you change the length (L) of the air column, resonance occurs at odd multiples of a quarter-wavelength LEMDA\/4\u003c\/span\u003e\u003c\/div\u003e\n                                                                                                                     \u003c\/li\u003e\n\u003c\/ol\u003e","brand":"scientifickart","offers":[{"title":"Default Title","offer_id":51610705461554,"sku":"OM-11020","price":1680.0,"currency_code":"INR","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0951\/6561\/2338\/files\/resonancetubeexperiment.png?v=1787144761","url":"https:\/\/scientifickart.com\/products\/to-find-the-speed-of-sound-in-air-at-room-temperature-using-a-resonance-tube-by-two-resonance-positions","provider":"scientifickart","version":"1.0","type":"link"}