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: \[ \boxed{60 \, \text{cm}}. \]
For \( \alpha, \beta, \gamma \in \mathbb{R} \), if \[ \lim_{x \to 0} \frac{x^2 \sin(\alpha x) + (\gamma - 1)e^{x^2}}{\sin(2x - \beta x)} = 3, \] then \( \beta + \gamma - \alpha \) is equal to:

In the first configuration (1) as shown in the figure, four identical charges \( q_0 \) are kept at the corners A, B, C and D of square of side length \( a \). In the second configuration (2), the same charges are shifted to mid points C, E, H, and F of the square. If \( K = \frac{1}{4\pi \epsilon_0} \), the difference between the potential energies of configuration (2) and (1) is given by: