Given:
- Initial resonating length, \( L = 90 \, \text{cm} \)
- Initial fundamental frequency, \( f_0 = 400 \, \text{Hz} \)
- New fundamental frequency, \( f' = 600 \, \text{Hz} \)
Step 1: Relation Between Frequency and Length
The fundamental frequency of a vibrating string is given by:
\[ f_0 = \frac{v}{2L}, \]
where:
- \( v \) is the wave speed,
- \( L \) is the length of the wire.
For the same tension, the wave speed \( v \) remains constant.
Step 2: Expressing New Length in Terms of Frequency
Let the new resonating length be \( L' \) for the frequency \( f' \). The new fundamental frequency is given by:
\[ f' = \frac{v}{2L'}. \]
Dividing the two equations:
\[ \frac{f'}{f_0} = \frac{L}{L'}. \]
Rearranging to find \( L' \):
\[ L' = L \times \frac{f_0}{f'}. \]
Step 3: Substituting the Given Values
Substituting the values:
\[ L' = 90 \times \frac{400}{600}. \]
Simplifying:
\[ L' = 90 \times \frac{2}{3} = 60 \, \text{cm}. \]
Therefore, the new resonating length of the wire is \( 60 \, \text{cm} \).
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 one focus of the hyperbola \( H : \dfrac{x^2}{a^2} - \dfrac{y^2}{b^2} = 1 \) be at \( (\sqrt{10}, 0) \) and the corresponding directrix be \( x = \dfrac{9}{\sqrt{10}} \). If \( e \) and \( l \) respectively are the eccentricity and the length of the latus rectum of \( H \), then \( 9 \left(e^2 + l \right) \) is equal to:
