两个同方向同频率简写振动方程分别为 x_1 = 0.6cos(2t + (5)/(6)pi) 和 x_2 = 0.8cos(2t - (1)/(6)pi) (SI制),则合振动方程为( )1. x = 0.1cos(2t + (1)/(3)pi) 2. x = 0.2cos(2t + (1)/(6)pi) 3. x = 0.2cos(2t - (1)/(6)pi) 4. x = 0.1cos(2t + (1)/(6)pi)
两个同方向同频率简写振动方程分别为 $ x_1 = 0.6\cos(2t + \frac{5}{6}\pi) $ 和 $ x_2 = 0.8\cos(2t - \frac{1}{6}\pi) $ (SI制),则合振动方程为( )
1. $ x = 0.1\cos(2t + \frac{1}{3}\pi) $
2. $ x = 0.2\cos(2t + \frac{1}{6}\pi) $
3. $ x = 0.2\cos(2t - \frac{1}{6}\pi) $
4. $ x = 0.1\cos(2t + \frac{1}{6}\pi) $
题目解答
答案
解析
本题考查同方向同频率简谐振动的合成知识。解题思路是先根据简谐振动合成公式求出合振动的振幅 $A$,再求出合振动的初相位 $\varphi$,最后得出合振动方程。
步骤一:求合振动的振幅 $A$
已知两个同方向同频率简谐振动方程分别为 $x_1 = A_1\cos(\omega t + \varphi_1)$ 和 $x_2 = A_2\cos(\omega t + \varphi_2)$,其中 $A_1 = 0.6$,$A_2 = 0.8$,$\omega = 2$,$\varphi_1 = \frac{5}{6}\pi$,$\varphi_2 = -\frac{1}{6}\pi$。
根据简谐振动合成公式 $A = \sqrt{A_1^2 + A_2^2 + 2 A_1 A_2 \cos(\varphi_2 - \varphi_1)}$,先计算 $\cos(\varphi_2 - \varphi_1)$:
$\varphi_2 - \varphi_1 = -\frac{1}{6}\pi - \frac{5}{6}\pi = -\pi$
$\cos(\varphi_2 - \varphi_1) = \cos(-\pi) = -1$
将 $A_1 = 0.6$,$A_2 = 0.8$,$\cos(\varphi_2 - \varphi_1) = -1$ 代入振幅公式可得:
$\begin{align*}A&=\sqrt{0.6^2 + 0.8^2 + 2\times 0.6\times 0.8\times (-1)}\\&=\sqrt{0.36 + 0.64 - 0.96}\\&=\sqrt{1 - 0.96}\\&=\sqrt{0.04}\\&= 0.2\end{align*}$
步骤二:求合振动的初相位 $\varphi$
根据公式 $\tan \varphi = \frac{A_1 \sin \varphi_1 + A_2 \sin \varphi_2}{A_1 \cos \varphi_1 + A_2 \cos \varphi_2}$,分别计算分子和分母:
- 计算分子 $A_1 \sin \varphi_1 + A_2 \sin \varphi_2$:
$A_1 \sin \varphi_1 = 0.6\times\sin(\frac{5}{6}\pi) = 0.6\times\frac{1}{2} = 0.3$
$A_2 \sin \varphi_2 = 0.8\times\sin(-\frac{1}{6}\pi) = 0.8\times(-\frac{1}{2}) = -0.4$
$A_1 \sin \varphi_1 + A_2 \sin \varphi_2 = 0.3 - 0.4 = -0.1$ - 计算分母 $A_1 \cos \varphi_1 + A_2 \cos \varphi_2$:
$A_1 \cos \varphi_1 = 0.6\times\cos(\frac{5}{6}\pi) = 0.6\times(-\frac{\sqrt{3}}{2}) = -0.3\sqrt{3}$
$A_2 \cos \varphi_2 = 0.8\times\cos(-\frac{1}{6}\pi) = 0.8\times\frac{\sqrt{3}}{2} = 0.4\sqrt{3}$
$A_1 \cos \varphi_1 + A_2 \cos \varphi_2 = -0.3\sqrt{3} + 0.4\sqrt{3} = 0.1\sqrt{3}$
将分子和分母的值代入 $\tan \varphi$ 公式可得:
$\tan \varphi = \frac{-0.1}{0.1\sqrt{3}} = -\frac{\sqrt{3}}{3}$
因为 $A_1 \cos \varphi_1 + A_2 \cos \varphi_2 = 0.1\sqrt{3} \gt 0$,$A_1 \sin \varphi_1 + A_2 \sin \varphi_2 = -0.1 \lt 0$,所以 $\varphi$ 在第四象限,可得 $\varphi = -\frac{\pi}{6}$。
步骤三:得出合振动方程
合振动方程为 $x = A\cos(\omega t + \varphi)$,将 $A = 0.2$,$\omega = 2$,$\varphi = -\frac{\pi}{6}$ 代入可得:
$x = 0.2\cos(2t - \frac{1}{6}\pi)$