Yatay parabolik at\u0131\u015f<\/strong> , yatay at\u0131\u015f<\/strong> veya yatay at\u0131\u015f<\/strong> , bir y\u00fckseklikten ba\u015flayan ve ba\u015flang\u0131\u00e7 h\u0131z\u0131 yatay olan parabol \u015feklinde bir harekettir.<\/p>\n Yatay parabolik at\u0131\u015f iki hareketin birle\u015fimidir: dikey hareket bir MRU’dur<\/a> ve yatay hareket bir MRUA’d\u0131r<\/a> .<\/p>\n \u00d6rne\u011fin bir binan\u0131n \u00e7at\u0131s\u0131ndan yatay olarak bir top f\u0131rlatmak yatay parabolik at\u0131\u015ft\u0131r. Top harekete belli bir y\u00fckseklikten ba\u015flar, ba\u015flang\u0131\u00e7 h\u0131z\u0131 tamamen yatayd\u0131r ve yer \u00e7ekiminden dolay\u0131 parabolik bir hareket yapar yani yatay parabolik bir at\u0131\u015ft\u0131r. <\/p>\n Fizikte yatay parabolik at\u0131\u015f\u0131n tan\u0131m\u0131n\u0131 g\u00f6rd\u00fckten sonra, bu t\u00fcr hareketin \u00f6zelliklerinin neler oldu\u011funa bakal\u0131m.<\/p>\n A\u015fa\u011f\u0131da yatay parabolik at\u0131\u015f i\u00e7in form\u00fcller (veya denklemler) bulunmaktad\u0131r. Bu form\u00fcller yatay parabolik draft problemlerini \u00e7\u00f6zmemize yard\u0131mc\u0131 olacakt\u0131r.<\/p>\n Yatay bir parabolik d\u00fczlemde, konumun yatay bile\u015feni, d\u00fczg\u00fcn do\u011frusal hareket (MRU) form\u00fcl\u00fcyle tan\u0131mlan\u0131rken, konumun dikey bile\u015feninin ifadesi, d\u00fczg\u00fcn h\u0131zland\u0131r\u0131lm\u0131\u015f do\u011frusal hareket (MRUA) form\u00fcl\u00fcd\u00fcr. Dolay\u0131s\u0131yla yatay bir parabolik at\u0131\u015f\u0131n y\u00f6r\u00fcngesini tan\u0131mlayan denklemler a\u015fa\u011f\u0131daki gibidir:<\/p>\n \n Alt\u0131n: <\/p>\n v\u00fccudun yatay koordinat\u0131d\u0131r. <\/span><\/li>\n v\u00fccudun dikey koordinat\u0131d\u0131r. <\/span><\/li>\n ba\u015flang\u0131\u00e7 h\u0131z\u0131d\u0131r. <\/span><\/li>\n ge\u00e7en s\u00fcredir. <\/span><\/li>\n v\u00fccudun ba\u015flang\u0131\u00e7 y\u00fcksekli\u011fidir. <\/span><\/li>\n de\u011feri 9,81 m\/ s2<\/sup> olan yer \u00e7ekimi ivmesidir.<\/span><\/li>\n<\/ul>\n Yatay parabolik at\u0131\u015fta h\u0131z\u0131n yatay bile\u015feni y\u00f6r\u00fcnge boyunca sabittir ve ba\u015flang\u0131\u00e7 h\u0131z\u0131n\u0131n de\u011ferine e\u015fde\u011ferdir.<\/p>\n \u00d6te yandan, yatay bir parabolik at\u0131\u015f\u0131n dikey bile\u015feni, d\u00fczg\u00fcn ivmeli do\u011frusal hareket denklemiyle tan\u0131mlan\u0131r. Yani h\u0131z\u0131n d\u00fc\u015fey bile\u015feni eksi yer \u00e7ekimi ivmesi \u00e7arp\u0131 ge\u00e7en zamana e\u015fittir.<\/p>\n \n Alt\u0131n: <\/p>\n h\u0131z\u0131n yatay bile\u015fenidir. <\/span><\/li>\n h\u0131z\u0131n dikey bile\u015fenidir. <\/span><\/li>\n ba\u015flang\u0131\u00e7 h\u0131z\u0131d\u0131r. <\/span><\/li>\n ge\u00e7en s\u00fcredir. <\/span><\/li>\n de\u011feri 9,81 m\/ s2<\/sup> olan yer \u00e7ekimi ivmesidir.<\/span><\/li>\n<\/ul>\n T\u00fcm yatay parabolik d\u00fczlemlerde cismin ivmesi her zaman ayn\u0131 de\u011ferdedir. \u0130vmenin yatay bile\u015feni s\u0131f\u0131rd\u0131r, ivmenin dikey bile\u015feni ise negatif i\u015faretli yer \u00e7ekiminin de\u011feridir (negatif bir ivme oldu\u011fu i\u00e7in).<\/p>\n \n Alt\u0131n: <\/p>\n ivmenin yatay bile\u015fenidir. <\/span><\/li>\n ivmenin dikey bile\u015fenidir. <\/span><\/li>\n de\u011feri 9,81 m\/ s2<\/sup> olan yer \u00e7ekimi ivmesidir.<\/span><\/li>\n<\/ul>\n U\u00e7u\u015f s\u00fcresi yatay parabolik at\u0131\u015f yapan v\u00fccudun yere de\u011fmesi i\u00e7in ge\u00e7en s\u00fcredir. Dolay\u0131s\u0131yla u\u00e7u\u015f s\u00fcresi, cismin parabole ba\u015flad\u0131\u011f\u0131 andan yere \u00e7arpt\u0131\u011f\u0131 ana kadar ge\u00e7en s\u00fcredir.<\/p>\n Dolay\u0131s\u0131yla yatay bir parabolik at\u0131\u015f\u0131n u\u00e7u\u015f s\u00fcresini hesaplama form\u00fcl\u00fc a\u015fa\u011f\u0131daki gibidir:<\/p>\n \n Alt\u0131n: <\/p>\n u\u00e7u\u015f zaman\u0131d\u0131r. <\/span><\/li>\n v\u00fccudun ba\u015flang\u0131\u00e7 y\u00fcksekli\u011fidir. <\/span><\/li>\n de\u011feri 9,81 m\/ s2<\/sup> olan yer \u00e7ekimi ivmesidir. <\/span><\/li>\n<\/ul>\n V\u00fccut yere \u00e7arpt\u0131\u011f\u0131nda konumunun dikey koordinat\u0131 s\u0131f\u0131r olacakt\u0131r. Dolay\u0131s\u0131yla u\u00e7u\u015f s\u00fcresini hesaplamak i\u00e7in yatay parabolik at\u0131\u015f\u0131n dikey konumu denklemini s\u0131f\u0131ra e\u015fitlemeniz ve ard\u0131ndan zaman denklemini \u00e7\u00f6zmeniz gerekir. <\/p>\n \n \n \n \n \n Maksimum yatay menzile, u\u00e7u\u015f s\u00fcresine e\u015fde\u011fer bir anda, g\u00f6vdenin yere de\u011fmesiyle ula\u015f\u0131lacakt\u0131r. Bu nedenle, yatay menzili hesaplamak i\u00e7in \u00f6ncelikle u\u00e7u\u015f s\u00fcresi al\u0131nmal\u0131 ve daha sonra u\u00e7u\u015f s\u00fcresi de\u011feri, yatay parabolik at\u0131\u015f\u0131n yatay konum denkleminde de\u011fi\u015ftirilmelidir.<\/p>\n \n Alt\u0131n: <\/p>\n maksimum yatay aral\u0131kt\u0131r. <\/span><\/li>\n ba\u015flang\u0131\u00e7 h\u0131z\u0131d\u0131r. <\/span><\/li>\n u\u00e7u\u015f zaman\u0131d\u0131r. <\/span><\/li>\n<\/ul>\n \u00d6zetle size yatay parabolik at\u0131\u015f i\u00e7in t\u00fcm form\u00fcllerin bulundu\u011fu bir tablo b\u0131rak\u0131yoruz: <\/p>\n A\u00e7\u0131klanan kavramlar\u0131 daha iyi \u00f6z\u00fcmsemek i\u00e7in a\u015fa\u011f\u0131da ad\u0131m ad\u0131m yatay parabolik at\u0131\u015f egzersizi bulacaks\u0131n\u0131z.<\/p>\n U\u00e7u\u015f s\u00fcresini bulmak i\u00e7in yukar\u0131da g\u00f6rd\u00fc\u011f\u00fcm\u00fcz form\u00fcl\u00fc uygulaman\u0131z yeterlidir:<\/p>\n \n U\u00e7u\u015f zaman\u0131n\u0131 bildi\u011fimizde, u\u00e7u\u015f zaman\u0131n\u0131n de\u011ferini pozisyonun yatay bile\u015feni denklemine koyarak maksimum yatay menzili belirleyebiliriz.<\/p>\n \n Son h\u0131z\u0131 hesaplamak i\u00e7in son anda yatay bile\u015fenini ve d\u00fc\u015fey bile\u015fenini belirlememiz gerekiyor. Yatay bile\u015fen y\u00f6r\u00fcnge boyunca sabittir ve ba\u015flang\u0131\u00e7 h\u0131z\u0131n\u0131n de\u011ferini olu\u015fturur.<\/p>\n \n \u00d6te yandan h\u0131z\u0131n d\u00fc\u015fey bile\u015fenini bulmak i\u00e7in buna kar\u015f\u0131l\u0131k gelen denklemi uygular\u0131z:<\/p>\n \n Dolay\u0131s\u0131yla h\u0131z\u0131n b\u00fcy\u00fckl\u00fc\u011f\u00fc, vekt\u00f6r bile\u015fenlerinin karelerinin toplam\u0131n\u0131n karek\u00f6k\u00fcne e\u015fittir: <\/p>\n \n Son olarak, yatay parabolik at\u0131\u015f ile e\u011fik parabolik at\u0131\u015f aras\u0131ndaki fark\u0131n ne oldu\u011funa bakal\u0131m, \u00e7\u00fcnk\u00fc bunlar kar\u0131\u015ft\u0131r\u0131labilecek iki t\u00fcr parabolik harekettir.<\/p>\n E\u011fik parabolik at\u0131\u015f,<\/strong> yatay olarak ilerlerken \u00f6nce y\u00fckselen sonra al\u00e7alan bir cismin ger\u00e7ekle\u015ftirdi\u011fi bu harekettir. Ba\u015fka bir deyi\u015fle, e\u011fik bir parabolik at\u0131\u015f\u0131n y\u00f6r\u00fcngesi tam bir parabold\u00fcr.<\/p>\n Yatay parabolik at\u0131\u015f ile e\u011fik parabolik at\u0131\u015f aras\u0131ndaki fark<\/strong> namlu \u00e7\u0131k\u0131\u015f h\u0131z\u0131d\u0131r. Yatay parabolik at\u0131\u015fta namlu \u00e7\u0131k\u0131\u015f h\u0131z\u0131 yatayd\u0131r, ancak e\u011fik parabolik at\u0131\u015fta namlu \u00e7\u0131k\u0131\u015f h\u0131z\u0131 yatay eksenle pozitif bir a\u00e7\u0131 olu\u015fturur.<\/p>\n B\u00f6ylece, yatay bir parabolik at\u0131\u015f\u0131n y\u00f6r\u00fcngesi tamamen yatay olarak ba\u015flarken, e\u011fik bir parabolik at\u0131\u015f\u0131n y\u00f6r\u00fcngesi, ba\u015flang\u0131\u00e7 h\u0131z\u0131n\u0131n yatay ve dikey bir bile\u015feni oldu\u011fundan yatay eksene bir a\u00e7\u0131yla ba\u015flar.<\/p>\n Ek olarak e\u011fer e\u011fik parabolik at\u0131\u015f yerde ba\u015fl\u0131yorsa, yatay parabolik at\u0131\u015f e\u011fik parabolik at\u0131\u015f\u0131n ortas\u0131ndan ba\u015flar. Dolay\u0131s\u0131yla yatay parabolik at\u0131\u015f\u0131n maksimum menzili ve u\u00e7u\u015f s\u00fcresi, e\u011fik parabolik at\u0131\u015f\u0131n maksimum menzili ve u\u00e7u\u015f s\u00fcresinin yar\u0131s\u0131 kadard\u0131r. <\/p>\n![\"yatay](\"https:\/\/physigeek.com\/wp-content\/uploads\/2023\/09\/lancement-de-tir-parabolique-horizontal.png\")
<\/figure>\n<\/span> Yatay parabolik at\u0131\u015f\u0131n \u00f6zellikleri<\/span><\/h2>\n
\n
<\/span> Yatay Parabolik At\u0131\u015f Form\u00fclleri<\/span><\/h2>\n
<\/span> Konum<\/span><\/h3>\n
![\"\\begin{cases}x=v_0\\cdot](\"https:\/\/physigeek.com\/wp-content\/ql-cache\/quicklatex.com-7c778eda7ac01cd4c754ec97d99f3b28_l3.png\" "\\"Rendered")
<\/p>\n<\/p>\n\n
![\"x\"](\"https:\/\/physigeek.com\/wp-content\/ql-cache\/quicklatex.com-7e5fbfa0bbbd9f3051cd156a0f1b5e31_l3.png\" "\\"Rendered")
<\/p>\n![\"y\"](\"https:\/\/physigeek.com\/wp-content\/ql-cache\/quicklatex.com-38461fc041e953482219abf5d4cce1cb_l3.png\" "\\"Rendered")
<\/p>\n![\"v_0\"](\"https:\/\/physigeek.com\/wp-content\/ql-cache\/quicklatex.com-033c1c43e83708a4a975dedd88f197a8_l3.png\" "\\"Rendered")
<\/p>\n![\"t\"](\"https:\/\/physigeek.com\/wp-content\/ql-cache\/quicklatex.com-fd9cb27edab3f0a8a249bc80cc9c6ee2_l3.png\" "\\"Rendered")
<\/p>\n![\"h\"](\"https:\/\/physigeek.com\/wp-content\/ql-cache\/quicklatex.com-2ce27f7d2d82e3b238176ec7e7ee9118_l3.png\" "\\"Rendered")
<\/p>\n![\"g\"](\"https:\/\/physigeek.com\/wp-content\/ql-cache\/quicklatex.com-e88010d25c51c0c42c505ee1004ed182_l3.png\" "\\"Rendered")
<\/p>\n<\/span> H\u0131z<\/span><\/h3>\n
![\"\\begin{cases}v_x=v_0](\"https:\/\/physigeek.com\/wp-content\/ql-cache\/quicklatex.com-923c94b2f351c8a83b26edb8bac9164b_l3.png\" "\\"Rendered")
<\/p>\n<\/p>\n\n
![\"v_x\"](\"https:\/\/physigeek.com\/wp-content\/ql-cache\/quicklatex.com-49b889f48d662e0aaa8d7cb4fe10f013_l3.png\" "\\"Rendered")
<\/p>\n![\"v_y\"](\"https:\/\/physigeek.com\/wp-content\/ql-cache\/quicklatex.com-5f9cca35a3ff6c43b956a6f9fe4e3921_l3.png\" "\\"Rendered")
<\/p>\n<\/p>\n<\/p>\n<\/p>\n<\/span> H\u0131zlanma<\/span><\/h3>\n
![\"\\begin{cases}a_x=0](\"https:\/\/physigeek.com\/wp-content\/ql-cache\/quicklatex.com-b317db933cced3fd619deeff201818c8_l3.png\" "\\"Rendered")
<\/p>\n<\/p>\n\n
![\"a_x\"](\"https:\/\/physigeek.com\/wp-content\/ql-cache\/quicklatex.com-9eccaa1194e3cd8a77d62f4a2fd89a51_l3.png\" "\\"Rendered")
<\/p>\n![\"a_y\"](\"https:\/\/physigeek.com\/wp-content\/ql-cache\/quicklatex.com-774db4a74587d8bf0c9a33ba6b3db0d3_l3.png\" "\\"Rendered")
<\/p>\n<\/p>\n<\/span> U\u00e7u\u015f zaman\u0131<\/span><\/h3>\n
![\"\\displaystyle](\"https:\/\/physigeek.com\/wp-content\/ql-cache\/quicklatex.com-319194c7a708eb2fa52ef3b34624a5ff_l3.png\" "\\"Rendered")
<\/p>\n<\/p>\n\n
![\"t_{flight}\"](\"https:\/\/physigeek.com\/wp-content\/ql-cache\/quicklatex.com-bd24a64e7d49c4ad9d16a92a468d51f2_l3.png\" "\\"Rendered")
<\/p>\n<\/p>\n<\/p>\n![\"y=h](\"https:\/\/physigeek.com\/wp-content\/ql-cache\/quicklatex.com-2ae71e3ad8efaa87d2cf99e31908530f_l3.png\" "\\"Rendered")
<\/p>\n<\/p>\n![\"0=h](\"https:\/\/physigeek.com\/wp-content\/ql-cache\/quicklatex.com-7854e3c3d9a1c8173b868c63ce4bcb85_l3.png\" "\\"Rendered")
<\/p>\n<\/p>\n![\"\\cfrac{1}{2}\\cdot](\"https:\/\/physigeek.com\/wp-content\/ql-cache\/quicklatex.com-32dd191b224eb6a2340a95a1d2a57ded_l3.png\" "\\"Rendered")
<\/p>\n<\/p>\n![\"t_{vol}^2=\\cfrac{2h}{g}\"](\"https:\/\/physigeek.com\/wp-content\/ql-cache\/quicklatex.com-adef29e16bcc19813ea6a7034698027c_l3.png\" "\\"Rendered")
<\/p>\n<\/p>\n<\/p>\n<\/p>\n<\/span> Yatay kapsam<\/span><\/h3>\n
![\"](\"https:\/\/physigeek.com\/wp-content\/ql-cache\/quicklatex.com-3daa5420bc4156b383762b58a0e8cc79_l3.png\" "\\"Rendered")
<\/p>\n<\/p>\n\n
![\"x_{m\\'ax}\"](\"https:\/\/physigeek.com\/wp-content\/ql-cache\/quicklatex.com-96befedb14fc2622547c54ae1f9fc906_l3.png\" "\\"Rendered")
<\/p>\n<\/p>\n<\/p>\n<\/span> Yatay Parabolik Taslak Form\u00fcllerin \u00d6zeti<\/span><\/h3>\n
![\"yatay](\"https:\/\/physigeek.com\/wp-content\/uploads\/2023\/09\/formules-paraboliques-horizontales.png\")
<\/figure>\n<\/span> \u00c7\u00f6z\u00fclm\u00fc\u015f yatay parabolik at\u0131\u015f al\u0131\u015ft\u0131rmas\u0131<\/span><\/h2>\n
\n
\n
![\"\\begin{aligned}\\displaystyle](\"https:\/\/physigeek.com\/wp-content\/ql-cache\/quicklatex.com-1ac5d065ded030390562ce814b72dd1e_l3.png\" "\\"Rendered")
<\/p>\n<\/p>\n![\"\\begin{aligned}x_{m\\'ax}&=v_0\\cdot](\"https:\/\/physigeek.com\/wp-content\/ql-cache\/quicklatex.com-866c53030ef8b4738e3fa18a4553bcdf_l3.png\" "\\"Rendered")
<\/p>\n<\/p>\n![\"v_x=v_0=6](\"https:\/\/physigeek.com\/wp-content\/ql-cache\/quicklatex.com-80721b6f97cfa44a795ec3e11c336bf7_l3.png\" "\\"Rendered")
<\/p>\n<\/p>\n![\"\\begin{aligned}v_{y_f}&=-g\\cdot](\"https:\/\/physigeek.com\/wp-content\/ql-cache\/quicklatex.com-1a07841e4f02139417f0a340a02d5738_l3.png\" "\\"Rendered")
<\/p>\n<\/p>\n![\"\\begin{aligned}|v_f|&=\\sqrt{v_x^2+v_{y_f}^2}\\\\[2ex]|v_f|&=\\sqrt{6^2+(-12,6)](\"https:\/\/physigeek.com\/wp-content\/ql-cache\/quicklatex.com-36f3b2b6bf5f5864c1bb969f89eca196_l3.png\" "\\"Rendered")
<\/p>\n<\/p>\n<\/span> Yatay parabolik at\u0131\u015f ve e\u011fik parabolik at\u0131\u015f<\/span><\/h2>\n
![\"yatay](\"https:\/\/physigeek.com\/wp-content\/uploads\/2023\/09\/tir-parabolique-horizontal-et-tir-parabolique-oblique.png\")
<\/figure>\n