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15S: التذبذبات (ملخص)
https://query.libretexts.org/%D8%A7%D9%84%D9%84%D8%BA%D8%A9_%D8%A7%D9%84%D8%B9%D8%B1%D8%A8%D9%8A%D8%A9/-_____(OpenStax)/15%3A_%D8%A7%D9%84%D8%AA%D8%B0%D8%A8%D8%B0%D8%A8%D8%A7%D8%AA/15.S%3A_%D8%A7%D9%84%D8%AA%D8%B0%D8%A8%D8%B0%D8%A8%D8%A7%D8%AA_(%D9%85%D9%84%D8%AE%D8%B5)
يتم إعطاء السرعة بواسطة v (t) = -A $\omega$ sin ( $\omega t + \phi$ ) = -v max sin ( $\omega t + \phi$ )، حيث v max = A $\omega$ = A $\sqrt{\frac{k}{m}}$ . يتم إعطاء التسارع بواسطة a (t) = -A\(\omeg...يتم إعطاء السرعة بواسطة v (t) = -A $\omega$ sin ( $\omega t + \phi$ ) = -v max sin ( $\omega t + \phi$ )، حيث v max = A $\omega$ = A $\sqrt{\frac{k}{m}}$ . يتم إعطاء التسارع بواسطة a (t) = -A $\omega^{2}$ cos ( $\omega t + \phi$ ) = -a max cos ( $\omega t + \phi$ )، حيث الحد الأقصى = A $\omega^{2}$ = A $\frac{k}{m}$ .
15.S: oscillations (muhtasari)
https://query.libretexts.org/Kiswahili/Chuo_Kikuu_Fizikia_I_-_Mitambo%2C_Sauti%2C_oscillations%2C_na_Waves_(OpenStax)/15%3A_Kufutwa/15.S%3A_oscillations_(muhtasari)
mzunguko angular $\omega$ , kipindi T, na frequency f ya oscillator rahisi harmonic hutolewa na $\omega = \sqrt{\frac{k}{m}}$ $\pi \sqrt{\frac{m}{k}}$ , T = 2 $\frac{1}{2 \pi} \sqrt{\frac{k}{m}}$ , n...mzunguko angular $\omega$ , kipindi T, na frequency f ya oscillator rahisi harmonic hutolewa na $\omega = \sqrt{\frac{k}{m}}$ $\pi \sqrt{\frac{m}{k}}$ , T = 2 $\frac{1}{2 \pi} \sqrt{\frac{k}{m}}$ , na f =, ambapo m ni wingi wa mfumo na k ni nguvu ya mara kwa mara. Aina rahisi ya oscillations ni kuhusiana na mifumo ambayo inaweza kuelezwa na sheria ya Hooke, F = -kx, ambapo F ni nguvu ya kurejesha, x ni makazi yao kutoka usawa au deformation, na k ni nguvu ya mara kwa mara ya mfumo.
15.S : Oscillations (résumé)
https://query.libretexts.org/Francais/Physique_universitaire_I_-_M%C3%A9canique%2C_son%2C_oscillations_et_ondes_(OpenStax)/15%3A_Oscillations/15.S%3A_Oscillations_(r%C3%A9sum%C3%A9)
Une masse m suspendue par un fil de longueur L et de masse négligeable est un simple pendule et subit une SHM pour des amplitudes inférieures à environ 15°. La période d'un pendule simple est T = 2\(\...Une masse m suspendue par un fil de longueur L et de masse négligeable est un simple pendule et subit une SHM pour des amplitudes inférieures à environ 15°. La période d'un pendule simple est T = 2 $\pi \sqrt{\frac{L}{g}}$ , où L est la longueur de la corde et g est l'accélération due à la gravité.
15.S：振荡（摘要）
https://query.libretexts.org/%E7%AE%80%E4%BD%93%E4%B8%AD%E6%96%87/%E5%A4%A7%E5%AD%A6%E7%89%A9%E7%90%86%E5%AD%A6_I-%E5%8A%9B%E5%AD%A6%E3%80%81%E5%A3%B0%E9%9F%B3%E3%80%81%E6%8C%AF%E8%8D%A1%E5%92%8C%E6%B3%A2%E6%B5%AA_(OpenStax)/15%3A_%E6%8C%AF%E8%8D%A1/15.S%3A_15.S%EF%BC%9A%E6%8C%AF%E8%8D%A1%EF%BC%88%E6%91%98%E8%A6%81%EF%BC%89
速度由 v (t) =-A $\omega$ sin ( $\omega t + \phi$ ) =-v max sin ( $\omega t + \phi$ ) 给出，其中 v max = A $\omega$ = A $\sqrt{\frac{k}{m}}$ 。加速度由 a (t) =-A $\omega^{2}$ cos ( $\omega t + \phi$ ) =-a max ...速度由 v (t) =-A $\omega$ sin ( $\omega t + \phi$ ) =-v max sin ( $\omega t + \phi$ ) 给出，其中 v max = A $\omega$ = A $\sqrt{\frac{k}{m}}$ 。加速度由 a (t) =-A $\omega^{2}$ cos ( $\omega t + \phi$ ) =-a max cos ( $\omega t + \phi$ ) 给出，其中 a max = A $\omega^{2}$ = A $\frac{k}{m}$ 。假设一个半径为 A 的圆，以恒定角速度移动 $\omega$ 。圆边上的点以 v max = A 的恒定切向速度移动 $\omega$ 。半径在 x 轴上的投影为 x (t) = Acos ( $\omega$ t + $\phi$ )，其中 ( $\phi$ ) 是相移。切向速度的 x 分量为 v (t) = −A $\omega$ sin ( $\omega$ t + $\phi$ )。
15.S: Oscilações (resumo)
https://query.libretexts.org/Idioma_Portugues/Fisica_Universitaria_I_-_Mecanica_Som_Oscilacoes_e_Ondas_(OpenStax)/15%3A_Oscilacoes/15.S%3A_Oscila%C3%A7%C3%B5es_(resumo)
A frequência angular $\omega$ , o período T e a frequência f de um oscilador harmônico simples são dados por $\omega = \sqrt{\frac{k}{m}}$ , T = 2 $\pi \sqrt{\frac{m}{k}}$ e f =\(\frac{1}{2 \pi} \sqr...A frequência angular $\omega$ , o período T e a frequência f de um oscilador harmônico simples são dados por $\omega = \sqrt{\frac{k}{m}}$ , T = 2 $\pi \sqrt{\frac{m}{k}}$ e f = $\frac{1}{2 \pi} \sqrt{\frac{k}{m}}$ , onde m é a massa do sistema e k é a força constante.