The block moves in a circular path due to the tension in the spring. This tension provides the necessary centripetal force for circular motion. The centripetal force is given by:
\( F_c = m \omega^2 r \)
where \( m \) is the mass, \( \omega \) is the angular velocity, and \( r \) is the radius of the circular path.
The tension in the spring is given by Hooke's Law:
\( T = kx \)
where \( k \) is the spring constant and \( x \) is the extension of the spring.
The radius of the circular path is the original length of the spring (\( l \)) plus the extension (\( x \)): \( r = l + x \). The tension in the spring provides the centripetal force, so:
\( kx = m \omega^2 (l + x) \)
Given: \( m = 100 \text{ g} = 0.1 \text{ kg} \), \( k = 7.5 \text{ N/m} \), \( l = 20 \text{ cm} = 0.2 \text{ m} \), and \( \omega = 5 \text{ rad/s} \). Substituting these values:
\( 7.5x = 0.1 \times (5)^2 \times (0.2 + x) \)
\( 7.5x = 0.1 \times 25 \times (0.2 + x) \)
\( 7.5x = 2.5 (0.2 + x) \)
\( 7.5x = 0.5 + 2.5x \)
\( 5x = 0.5 \)
\( x = 0.1 \text{ m} \)
Now that we know the extension \( x \), we can calculate the tension in the spring:
\( T = kx = 7.5 \times 0.1 = 0.75 \text{ N} \)
The tension in the spring is 0.75 N (Option 1).
Let $ P_n = \alpha^n + \beta^n $, $ n \in \mathbb{N} $. If $ P_{10} = 123,\ P_9 = 76,\ P_8 = 47 $ and $ P_1 = 1 $, then the quadratic equation having roots $ \alpha $ and $ \frac{1}{\beta} $ is: