The fundamental frequency (\( f \)) of a vibrating string is given by: \[ f = \frac{v}{2L}, \] where: \item \( f \) is the frequency, \item \( v \) is the wave velocity, \item \( L \) is the length of the string.
Step 1: Relation between frequencies and lengths. For the initial string length (\( L \)) and frequency (\( f_1 = 120 \, \text{Hz} \)): \[ f_1 = \frac{v}{2L}. \] For the new string length (\( L' \)) and frequency (\( f_2 = 180 \, \text{Hz} \)): \[ f_2 = \frac{v}{2L'}. \] Taking the ratio of the two frequencies: \[ \frac{f_2}{f_1} = \frac{L}{L'}. \] Substitute \( f_1 = 120 \, \text{Hz} \) and \( f_2 = 180 \, \text{Hz} \): \[ \frac{180}{120} = \frac{L}{L'}. \] Simplify: \[ \frac{3}{2} = \frac{L}{L'}. \] Rearrange to solve for \( L' \): \[ L' = \frac{2}{3} L. \]
Step 2: Substitute the initial length. Given \( L = 90 \, \text{cm} \): \[ L' = \frac{2}{3} \cdot 90 = 60 \, \text{cm}. \]
Final Answer: The new string length is: \[ \boxed{60 \, \text{cm}}. \]
Two plane polarized light waves combine at a certain point, whose "E" components are: \[ E_1 = E_0 \sin \omega t, \quad E_2 = E_0 \sin \left( \omega t + \frac{\pi}{3} \right) \] Find the amplitude of the resultant wave.

Let \( a \in \mathbb{R} \) and \( A \) be a matrix of order \( 3 \times 3 \) such that \( \det(A) = -4 \) and \[ A + I = \begin{bmatrix} 1 & a & 1 \\ 2 & 1 & 0 \\ a & 1 & 2 \end{bmatrix} \] where \( I \) is the identity matrix of order \( 3 \times 3 \).
If \( \det\left( (a + 1) \cdot \text{adj}\left( (a - 1) A \right) \right) \) is \( 2^m 3^n \), \( m, n \in \{ 0, 1, 2, \dots, 20 \} \), then \( m + n \) is equal to: