To solve the problem, we begin by understanding the relationship between the frequency of oscillations and the mass attached to the spring, given by the formula for the frequency of a mass-spring system: \( f = \frac{1}{2\pi}\sqrt{\frac{k}{m}} \), where \( k \) is the spring constant and \( m \) is the mass.
For mass \( m \), the frequency is \( f_1 = \frac{1}{2\pi} \sqrt{\frac{k}{m}} \).
For mass \( 9m \), the frequency is \( f_2 = \frac{1}{2\pi} \sqrt{\frac{k}{9m}} = \frac{1}{2\pi} \frac{1}{3} \sqrt{\frac{k}{m}} = \frac{1}{3} \cdot f_1 \).
Thus, \(\frac{f_1}{f_2} = \frac{f_1}{\frac{1}{3}f_1} = 3\).
Hence, the value of \(\frac{f_1}{f_2}\) is clearly \( 3 \), which falls within the given range 3,3.
Given: - Mass of first system: \( m \) - Mass of second system: \( 9m \) - Frequencies: \( f_1 \) and \( f_2 \)
The frequency of oscillation of a mass-spring system is given by:
\[ f = \frac{1}{2\pi} \sqrt{\frac{k}{m}} \]
where \( k \) is the spring constant and \( m \) is the mass.
For the first system with mass \( m \):
\[ f_1 = \frac{1}{2\pi} \sqrt{\frac{k}{m}} \]
For the second system with mass \( 9m \):
\[ f_2 = \frac{1}{2\pi} \sqrt{\frac{k}{9m}} = \frac{1}{2\pi} \cdot \frac{1}{3} \sqrt{\frac{k}{m}} = \frac{f_1}{3} \]
\[ \frac{f_1}{f_2} = \frac{f_1}{\frac{f_1}{3}} = 3 \]
Conclusion: The value of \( \frac{f_1}{f_2} \) is \( 3 \).
Two simple pendulums having lengths $l_{1}$ and $l_{2}$ with negligible string mass undergo angular displacements $\theta_{1}$ and $\theta_{2}$, from their mean positions, respectively. If the angular accelerations of both pendulums are same, then which expression is correct?
A particle is subjected to simple harmonic motions as: $ x_1 = \sqrt{7} \sin 5t \, \text{cm} $ $ x_2 = 2 \sqrt{7} \sin \left( 5t + \frac{\pi}{3} \right) \, \text{cm} $ where $ x $ is displacement and $ t $ is time in seconds. The maximum acceleration of the particle is $ x \times 10^{-2} \, \text{m/s}^2 $. The value of $ x $ is:
Let \( y^2 = 12x \) be the parabola and \( S \) its focus. Let \( PQ \) be a focal chord of the parabola such that \( (SP)(SQ) = \frac{147}{4} \). Let \( C \) be the circle described by taking \( PQ \) as a diameter. If the equation of the circle \( C \) is: \[ 64x^2 + 64y^2 - \alpha x - 64\sqrt{3}y = \beta, \] then \( \beta - \alpha \) is equal to:
The dimensions of a physical quantity \( \epsilon_0 \frac{d\Phi_E}{dt} \) are similar to [Symbols have their usual meanings]
The expression given below shows the variation of velocity \( v \) with time \( t \): \[ v = \frac{At^2 + Bt}{C + t} \] The dimension of \( A \), \( B \), and \( C \) is:
