<\/span> \u0130vmenin sabit olmas\u0131 ne anlama geliyor?<\/span><\/h2>\n E\u011fer bir cisim sabit ivmeyle hareket ediyorsa bu onun h\u0131z\u0131n\u0131n zaman i\u00e7inde s\u00fcrekli de\u011fi\u015fti\u011fi anlam\u0131na gelir.<\/strong> Ba\u015fka bir deyi\u015fle, bir cismin ivmesinin sabit olmas\u0131, h\u0131z\u0131n\u0131n zamana g\u00f6re do\u011frusal olarak artmas\u0131 veya azalmas\u0131 anlam\u0131na gelir.<\/p>\n \u00d6rne\u011fin bir cisim 2 m\/ s2<\/sup> sabit ivmeyle ileri do\u011fru hareket ediyorsa bu, h\u0131z\u0131n\u0131n her saniye 2 m\/s artaca\u011f\u0131 anlam\u0131na gelir. Yani hareketsiz halden ba\u015flarsa, bir saniye sonra h\u0131z\u0131 2 m\/s, iki saniye sonra 4 m\/s, \u00fc\u00e7 saniye sonra 6 m\/s vb. olacakt\u0131r.<\/p>\n \u0130vmenin sadece h\u0131z\u0131n b\u00fcy\u00fckl\u00fc\u011f\u00fcn\u00fc de\u011fi\u015ftirmekle kalmay\u0131p ayn\u0131 zamanda h\u0131z\u0131n y\u00f6n\u00fcn\u00fc de de\u011fi\u015ftirebilece\u011fi unutulmamal\u0131d\u0131r. D\u00fczg\u00fcn dairesel hareket (MCU)<\/a> gibi hareketler, h\u0131z mod\u00fcl\u00fcn\u00fc hareket boyunca sabit tutar ancak y\u00f6n\u00fc de\u011fi\u015fir, dolay\u0131s\u0131yla d\u00f6n\u00fc\u015fler sabit h\u0131zda yap\u0131l\u0131r. <\/p>\n \u27a4<\/span> Bak\u0131n\u0131z:<\/strong> H\u0131z nedir?<\/a><\/div>\n Dolay\u0131s\u0131yla serbest d\u00fc\u015f\u00fc\u015fle al\u00e7alan bir cisim, sabit ivmeli harekete bir \u00f6rnektir, \u00e7\u00fcnk\u00fc de\u011feri sabit olan (g=9.81 m\/s 2<\/sup> ) cisme yaln\u0131zca yer \u00e7ekimi ivmesi etki eder (hava ile s\u00fcrt\u00fcnmeyi ihmal eder). ). <\/p>\n<\/span> Sabit h\u0131zlanma hareketlerine \u00f6rnekler<\/span><\/h2>\n Sabit ivme kavram\u0131n\u0131 anlamay\u0131 tamamlamak i\u00e7in, y\u00f6r\u00fcnge boyunca ivmesi sabit olan hareketlerin \u00f6rneklerini a\u015fa\u011f\u0131da g\u00f6rebilirsiniz.<\/p>\n
\n- D\u00fczg\u00fcn h\u0131zland\u0131r\u0131lm\u0131\u015f do\u011frusal hareket<\/a><\/li>\n
- Parabolik hareket<\/a><\/li>\n
- Yatay ba\u015flatma<\/a><\/li>\n
- Serbest d\u00fc\u015f\u00fc\u015f<\/a><\/li>\n
- Dikey \u00e7ekim<\/a> <\/li>\n<\/ul>\n
<\/span> Sabit ivmede hareket form\u00fclleri<\/span><\/h2>\n A\u015fa\u011f\u0131da size sabit ivmeli hareket form\u00fcllerinin (veya denklemlerinin) ne oldu\u011funu g\u00f6steriyoruz. Bu form\u00fcller bu t\u00fcr hareketlerin sorunlar\u0131n\u0131 \u00e7\u00f6zmenize olanak sa\u011flayacakt\u0131r.<\/p>\n
<\/span> Konum<\/span><\/h3>\n Hareketin ivmesi sabit oldu\u011funda, bir cismin konumu ba\u015flang\u0131\u00e7 konumu art\u0131 ba\u015flang\u0131\u00e7 h\u0131z\u0131 \u00e7arp\u0131 ge\u00e7en zaman art\u0131 ivmenin yar\u0131s\u0131 \u00e7arp\u0131 ge\u00e7en zaman\u0131n karesinin \u00e7arp\u0131m\u0131na e\u015fittir.<\/p>\n
B\u00f6ylece, sabit ivmeli bir hareketi tan\u0131mlayan cismin konumunu hesaplama form\u00fcl\u00fc<\/strong> a\u015fa\u011f\u0131daki gibidir:<\/p>\n\n
![\"x=x_0+v_0\\cdot](\"https:\/\/physigeek.com\/wp-content\/ql-cache\/quicklatex.com-12ff67c6c64f8517159c4c2274aa980e_l3.png\" "\\"Rendered")
<\/p>\n<\/p>\n
Alt\u0131n: <\/p>\n
\n- \n
![\"x\"](\"https:\/\/physigeek.com\/wp-content\/ql-cache\/quicklatex.com-7e5fbfa0bbbd9f3051cd156a0f1b5e31_l3.png\" "\\"Rendered")
<\/p>\n
v\u00fccudun konumudur. <\/span><\/li>\n
- \n
![\"x_0\"](\"https:\/\/physigeek.com\/wp-content\/ql-cache\/quicklatex.com-e6e1c3611728e9db0e52bb6485e06068_l3.png\" "\\"Rendered")
<\/p>\n
v\u00fccudun ba\u015flang\u0131\u00e7 pozisyonudur. <\/span><\/li>\n
- \n
![\"v_0\"](\"https:\/\/physigeek.com\/wp-content\/ql-cache\/quicklatex.com-033c1c43e83708a4a975dedd88f197a8_l3.png\" "\\"Rendered")
<\/p>\n
v\u00fccudun ba\u015flang\u0131\u00e7 h\u0131z\u0131d\u0131r. <\/span><\/li>\n
- \n
![\"t\"](\"https:\/\/physigeek.com\/wp-content\/ql-cache\/quicklatex.com-fd9cb27edab3f0a8a249bc80cc9c6ee2_l3.png\" "\\"Rendered")
<\/p>\n
v\u00fccut pozisyonunun hesapland\u0131\u011f\u0131 zamand\u0131r. <\/span><\/li>\n
- \n
![\"t_0\"](\"https:\/\/physigeek.com\/wp-content\/ql-cache\/quicklatex.com-c1a3f4a217f20d31e6f72a2f42a2e7dd_l3.png\" "\\"Rendered")
<\/p>\n
ba\u015flang\u0131\u00e7 an\u0131d\u0131r. <\/span><\/li>\n
- \n
![\"a\"](\"https:\/\/physigeek.com\/wp-content\/ql-cache\/quicklatex.com-0e55b0b3943237ccfc96979505679274_l3.png\" "\\"Rendered")
<\/p>\n
v\u00fccudun ivmesidir.<\/span><\/li>\n<\/ul>\n
<\/span> H\u0131z<\/span><\/h3>\n Bir cisim sabit ivmeyle hareket etti\u011finde, h\u0131z zamanla e\u015fit olarak de\u011fi\u015fir. Yani belirli bir zamandaki h\u0131z, ba\u015flang\u0131\u00e7 h\u0131z\u0131 art\u0131 cismin ivmesi \u00e7arp\u0131 ge\u00e7en zamana e\u015fittir.<\/p>\n
Bu nedenle, ivme sabitken h\u0131z\u0131 hesaplama form\u00fcl\u00fc<\/strong> \u015f\u00f6yledir:<\/p>\n\n
![\"v=v_0+a\\cdot](\"https:\/\/physigeek.com\/wp-content\/ql-cache\/quicklatex.com-56736742d1dc1fd0e737eca12cafe6b2_l3.png\" "\\"Rendered")
<\/p>\n<\/p>\n
Alt\u0131n: <\/p>\n
\n- \n
![\"v\"](\"https:\/\/physigeek.com\/wp-content\/ql-cache\/quicklatex.com-796872219106704832bd95ce08640b7b_l3.png\" "\\"Rendered")
<\/p>\n
belirli bir andaki v\u00fccudun h\u0131z\u0131d\u0131r. <\/span><\/li>\n
- \n
<\/p>\n
v\u00fccudun ba\u015flang\u0131\u00e7 h\u0131z\u0131d\u0131r. <\/span><\/li>\n
- \n
<\/p>\n
v\u00fccudun ivmesidir. <\/span><\/li>\n
- \n
<\/p>\n
v\u00fccut h\u0131z\u0131n\u0131n hesapland\u0131\u011f\u0131 and\u0131r. <\/span><\/li>\n
- \n
<\/p>\n
ba\u015flang\u0131\u00e7 an\u0131d\u0131r.<\/span><\/li>\n<\/ul>\n
\u00d6te yandan h\u0131z\u0131 v\u00fccut konumu ve ivmeyle ili\u015fkilendiren ba\u015fka bir form\u00fcl daha var. Bu form\u00fcl\u00fcn avantaj\u0131, zaman\u0131n orada g\u00f6r\u00fcnmemesidir, dolay\u0131s\u0131yla baz\u0131 sorunlar\u0131n \u00e7\u00f6z\u00fcm\u00fcnde faydal\u0131 olabilir.<\/p>\n
\n
![\"v^2=v_0^2+2\\cdot](\"https:\/\/physigeek.com\/wp-content\/ql-cache\/quicklatex.com-8a75aebd09f11cbfa42c33b94fde6867_l3.png\" "\\"Rendered")
<\/p>\n<\/p>\n
Alt\u0131n: <\/p>\n
\n- \n
<\/p>\n
v\u00fccudun h\u0131z\u0131d\u0131r. <\/span><\/li>\n
- \n
<\/p>\n
v\u00fccudun ba\u015flang\u0131\u00e7 h\u0131z\u0131d\u0131r. <\/span><\/li>\n
- \n
<\/p>\n
v\u00fccudun ivmesidir. <\/span><\/li>\n
- \n
<\/p>\n
h\u0131z\u0131n hesapland\u0131\u011f\u0131 andaki v\u00fccudun konumudur. <\/span><\/li>\n
- \n
<\/p>\n
v\u00fccudun ba\u015flang\u0131\u00e7 pozisyonudur.<\/span><\/li>\n<\/ul>\n
<\/span> H\u0131zlanma<\/span><\/h3>\n \u0130vme sabitse, h\u0131zdaki de\u011fi\u015fimin (\u0394v) zamandaki de\u011fi\u015fime (\u0394t) b\u00f6l\u00fcnmesiyle hesaplan\u0131r. Dolay\u0131s\u0131yla sabit ivmenin form\u00fcl\u00fc<\/strong> a=\u0394v\/\u0394t’dir.<\/p>\n\n
![\"a=\\cfrac{\\Delta](\"https:\/\/physigeek.com\/wp-content\/ql-cache\/quicklatex.com-2f2c6987b1994109ed1e24980e9b0bae_l3.png\" "\\"Rendered")
<\/p>\n<\/p>\n
Alt\u0131n: <\/p>\n
\n- \n
<\/p>\n
ivmedir. <\/span><\/li>\n
- \n
![\"\\Delta](\"https:\/\/physigeek.com\/wp-content\/ql-cache\/quicklatex.com-94ac7e028a0584ad0183447f9c0fe2f9_l3.png\" "\\"Rendered")
<\/p>\n
h\u0131z art\u0131\u015f\u0131d\u0131r. <\/span><\/li>\n
- \n
![\"\\Delta](\"https:\/\/physigeek.com\/wp-content\/ql-cache\/quicklatex.com-819ab50990df5adf82bea9dfa75ffff2_l3.png\" "\\"Rendered")
<\/p>\n
bir zaman art\u0131\u015f\u0131d\u0131r. <\/span><\/li>\n
- \n
![\"v_f\"](\"https:\/\/physigeek.com\/wp-content\/ql-cache\/quicklatex.com-5d8e0d73e36f7ffd98c73baf4bec8be0_l3.png\" "\\"Rendered")
<\/p>\n
son h\u0131zd\u0131r. <\/span><\/li>\n
- \n
![\"v_i\"](\"https:\/\/physigeek.com\/wp-content\/ql-cache\/quicklatex.com-c9928f5e418ac3466349509fd03bdead_l3.png\" "\\"Rendered")
<\/p>\n
ba\u015flang\u0131\u00e7 h\u0131z\u0131d\u0131r. <\/span><\/li>\n
- \n
![\"t_f\"](\"https:\/\/physigeek.com\/wp-content\/ql-cache\/quicklatex.com-82d36af17e232807e56da9ccdbbda0d8_l3.png\" "\\"Rendered")
<\/p>\n
son an\u0131m\u0131zd\u0131r. <\/span><\/li>\n
- \n
![\"t_i\"](\"https:\/\/physigeek.com\/wp-content\/ql-cache\/quicklatex.com-bf289b768173104db12fe7044c723db4_l3.png\" "\\"Rendered")
<\/p>\n
ba\u015flang\u0131\u00e7 an\u0131d\u0131r. <\/span><\/li>\n<\/ul>\n
<\/span> sabit h\u0131zlanma ve sabit h\u0131z<\/span><\/h2>\n Son olarak, sabit ivmeli bir hareket ile sabit h\u0131zl\u0131 bir hareket aras\u0131ndaki fark\u0131n ne oldu\u011funu g\u00f6rece\u011fiz, \u00e7\u00fcnk\u00fc bunlar fizikte \u00e7ok farkl\u0131 iki hareket t\u00fcr\u00fcn\u00fc ima eden iki kavramd\u0131r.<\/p>\n
Makale boyunca g\u00f6rd\u00fc\u011f\u00fcm\u00fcz gibi, sabit ivmeli hareket, cismin h\u0131z\u0131nda bir de\u011fi\u015fiklik meydana getirir. Daha do\u011frusu ivme sabitse h\u0131z zamanla do\u011frusal olarak de\u011fi\u015fir.<\/p>\n
\u00d6te yandan bir cismin h\u0131z\u0131n\u0131n sabit olmas\u0131 onun ivmesinin s\u0131f\u0131ra e\u015fit oldu\u011fu anlam\u0131na gelir. Fizikte ivme, birim zaman ba\u015f\u0131na h\u0131zdaki de\u011fi\u015fimi g\u00f6sterir, dolay\u0131s\u0131yla h\u0131z de\u011fi\u015fmezse ivme s\u0131f\u0131r olacakt\u0131r.<\/p>\n
G\u00f6rd\u00fc\u011f\u00fcn\u00fcz gibi ivme ve h\u0131z birbiriyle ili\u015fkilidir ve asl\u0131nda bu niceliklerden biri sabit oldu\u011funda di\u011feri \u00fczerinde sonu\u00e7lar do\u011furur. Daha fazlas\u0131n\u0131 \u00f6\u011frenmek i\u00e7in web sitemizde yer alan a\u015fa\u011f\u0131daki makaleyi okuyabilirsiniz: <\/p>\n
\u00d6rne\u011fin bir cisim 2 m\/ s2<\/sup> sabit ivmeyle ileri do\u011fru hareket ediyorsa bu, h\u0131z\u0131n\u0131n her saniye 2 m\/s artaca\u011f\u0131 anlam\u0131na gelir. Yani hareketsiz halden ba\u015flarsa, bir saniye sonra h\u0131z\u0131 2 m\/s, iki saniye sonra 4 m\/s, \u00fc\u00e7 saniye sonra 6 m\/s vb. olacakt\u0131r.<\/p>\n \u0130vmenin sadece h\u0131z\u0131n b\u00fcy\u00fckl\u00fc\u011f\u00fcn\u00fc de\u011fi\u015ftirmekle kalmay\u0131p ayn\u0131 zamanda h\u0131z\u0131n y\u00f6n\u00fcn\u00fc de de\u011fi\u015ftirebilece\u011fi unutulmamal\u0131d\u0131r. D\u00fczg\u00fcn dairesel hareket (MCU)<\/a> gibi hareketler, h\u0131z mod\u00fcl\u00fcn\u00fc hareket boyunca sabit tutar ancak y\u00f6n\u00fc de\u011fi\u015fir, dolay\u0131s\u0131yla d\u00f6n\u00fc\u015fler sabit h\u0131zda yap\u0131l\u0131r. <\/p>\n Dolay\u0131s\u0131yla serbest d\u00fc\u015f\u00fc\u015fle al\u00e7alan bir cisim, sabit ivmeli harekete bir \u00f6rnektir, \u00e7\u00fcnk\u00fc de\u011feri sabit olan (g=9.81 m\/s 2<\/sup> ) cisme yaln\u0131zca yer \u00e7ekimi ivmesi etki eder (hava ile s\u00fcrt\u00fcnmeyi ihmal eder). ). <\/p>\n Sabit ivme kavram\u0131n\u0131 anlamay\u0131 tamamlamak i\u00e7in, y\u00f6r\u00fcnge boyunca ivmesi sabit olan hareketlerin \u00f6rneklerini a\u015fa\u011f\u0131da g\u00f6rebilirsiniz.<\/p>\n A\u015fa\u011f\u0131da size sabit ivmeli hareket form\u00fcllerinin (veya denklemlerinin) ne oldu\u011funu g\u00f6steriyoruz. Bu form\u00fcller bu t\u00fcr hareketlerin sorunlar\u0131n\u0131 \u00e7\u00f6zmenize olanak sa\u011flayacakt\u0131r.<\/p>\n Hareketin ivmesi sabit oldu\u011funda, bir cismin konumu ba\u015flang\u0131\u00e7 konumu art\u0131 ba\u015flang\u0131\u00e7 h\u0131z\u0131 \u00e7arp\u0131 ge\u00e7en zaman art\u0131 ivmenin yar\u0131s\u0131 \u00e7arp\u0131 ge\u00e7en zaman\u0131n karesinin \u00e7arp\u0131m\u0131na e\u015fittir.<\/p>\n B\u00f6ylece, sabit ivmeli bir hareketi tan\u0131mlayan cismin konumunu hesaplama form\u00fcl\u00fc<\/strong> a\u015fa\u011f\u0131daki gibidir:<\/p>\n \n Alt\u0131n: <\/p>\n v\u00fccudun konumudur. <\/span><\/li>\n v\u00fccudun ba\u015flang\u0131\u00e7 pozisyonudur. <\/span><\/li>\n v\u00fccudun ba\u015flang\u0131\u00e7 h\u0131z\u0131d\u0131r. <\/span><\/li>\n v\u00fccut pozisyonunun hesapland\u0131\u011f\u0131 zamand\u0131r. <\/span><\/li>\n ba\u015flang\u0131\u00e7 an\u0131d\u0131r. <\/span><\/li>\n v\u00fccudun ivmesidir.<\/span><\/li>\n<\/ul>\n Bir cisim sabit ivmeyle hareket etti\u011finde, h\u0131z zamanla e\u015fit olarak de\u011fi\u015fir. Yani belirli bir zamandaki h\u0131z, ba\u015flang\u0131\u00e7 h\u0131z\u0131 art\u0131 cismin ivmesi \u00e7arp\u0131 ge\u00e7en zamana e\u015fittir.<\/p>\n Bu nedenle, ivme sabitken h\u0131z\u0131 hesaplama form\u00fcl\u00fc<\/strong> \u015f\u00f6yledir:<\/p>\n \n Alt\u0131n: <\/p>\n belirli bir andaki v\u00fccudun h\u0131z\u0131d\u0131r. <\/span><\/li>\n v\u00fccudun ba\u015flang\u0131\u00e7 h\u0131z\u0131d\u0131r. <\/span><\/li>\n v\u00fccudun ivmesidir. <\/span><\/li>\n v\u00fccut h\u0131z\u0131n\u0131n hesapland\u0131\u011f\u0131 and\u0131r. <\/span><\/li>\n ba\u015flang\u0131\u00e7 an\u0131d\u0131r.<\/span><\/li>\n<\/ul>\n \u00d6te yandan h\u0131z\u0131 v\u00fccut konumu ve ivmeyle ili\u015fkilendiren ba\u015fka bir form\u00fcl daha var. Bu form\u00fcl\u00fcn avantaj\u0131, zaman\u0131n orada g\u00f6r\u00fcnmemesidir, dolay\u0131s\u0131yla baz\u0131 sorunlar\u0131n \u00e7\u00f6z\u00fcm\u00fcnde faydal\u0131 olabilir.<\/p>\n \n Alt\u0131n: <\/p>\n v\u00fccudun h\u0131z\u0131d\u0131r. <\/span><\/li>\n v\u00fccudun ba\u015flang\u0131\u00e7 h\u0131z\u0131d\u0131r. <\/span><\/li>\n v\u00fccudun ivmesidir. <\/span><\/li>\n h\u0131z\u0131n hesapland\u0131\u011f\u0131 andaki v\u00fccudun konumudur. <\/span><\/li>\n v\u00fccudun ba\u015flang\u0131\u00e7 pozisyonudur.<\/span><\/li>\n<\/ul>\n \u0130vme sabitse, h\u0131zdaki de\u011fi\u015fimin (\u0394v) zamandaki de\u011fi\u015fime (\u0394t) b\u00f6l\u00fcnmesiyle hesaplan\u0131r. Dolay\u0131s\u0131yla sabit ivmenin form\u00fcl\u00fc<\/strong> a=\u0394v\/\u0394t’dir.<\/p>\n \n Alt\u0131n: <\/p>\n ivmedir. <\/span><\/li>\n h\u0131z art\u0131\u015f\u0131d\u0131r. <\/span><\/li>\n bir zaman art\u0131\u015f\u0131d\u0131r. <\/span><\/li>\n son h\u0131zd\u0131r. <\/span><\/li>\n ba\u015flang\u0131\u00e7 h\u0131z\u0131d\u0131r. <\/span><\/li>\n son an\u0131m\u0131zd\u0131r. <\/span><\/li>\n ba\u015flang\u0131\u00e7 an\u0131d\u0131r. <\/span><\/li>\n<\/ul>\n Son olarak, sabit ivmeli bir hareket ile sabit h\u0131zl\u0131 bir hareket aras\u0131ndaki fark\u0131n ne oldu\u011funu g\u00f6rece\u011fiz, \u00e7\u00fcnk\u00fc bunlar fizikte \u00e7ok farkl\u0131 iki hareket t\u00fcr\u00fcn\u00fc ima eden iki kavramd\u0131r.<\/p>\n Makale boyunca g\u00f6rd\u00fc\u011f\u00fcm\u00fcz gibi, sabit ivmeli hareket, cismin h\u0131z\u0131nda bir de\u011fi\u015fiklik meydana getirir. Daha do\u011frusu ivme sabitse h\u0131z zamanla do\u011frusal olarak de\u011fi\u015fir.<\/p>\n \u00d6te yandan bir cismin h\u0131z\u0131n\u0131n sabit olmas\u0131 onun ivmesinin s\u0131f\u0131ra e\u015fit oldu\u011fu anlam\u0131na gelir. Fizikte ivme, birim zaman ba\u015f\u0131na h\u0131zdaki de\u011fi\u015fimi g\u00f6sterir, dolay\u0131s\u0131yla h\u0131z de\u011fi\u015fmezse ivme s\u0131f\u0131r olacakt\u0131r.<\/p>\n G\u00f6rd\u00fc\u011f\u00fcn\u00fcz gibi ivme ve h\u0131z birbiriyle ili\u015fkilidir ve asl\u0131nda bu niceliklerden biri sabit oldu\u011funda di\u011feri \u00fczerinde sonu\u00e7lar do\u011furur. Daha fazlas\u0131n\u0131 \u00f6\u011frenmek i\u00e7in web sitemizde yer alan a\u015fa\u011f\u0131daki makaleyi okuyabilirsiniz: <\/p>\n<\/span> Sabit h\u0131zlanma hareketlerine \u00f6rnekler<\/span><\/h2>\n
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<\/span> Sabit ivmede hareket form\u00fclleri<\/span><\/h2>\n
<\/span> Konum<\/span><\/h3>\n
<\/p>\n<\/p>\n\n
<\/p>\n<\/p>\n<\/p>\n<\/p>\n<\/p>\n<\/p>\n<\/span> H\u0131z<\/span><\/h3>\n
<\/p>\n<\/p>\n\n
<\/p>\n<\/p>\n<\/p>\n<\/p>\n<\/p>\n<\/p>\n<\/p>\n\n
<\/p>\n<\/p>\n<\/p>\n<\/p>\n<\/p>\n<\/span> H\u0131zlanma<\/span><\/h3>\n
<\/p>\n<\/p>\n\n
<\/p>\n<\/p>\n<\/p>\n<\/p>\n<\/p>\n<\/p>\n<\/p>\n<\/span> sabit h\u0131zlanma ve sabit h\u0131z<\/span><\/h2>\n