A force of 49 N acts tangentially at the highest point of a sphere (solid) of mass 20 kg, kept on a rough horizontal plane. If the sphere rolls without slipping, then the acceleration of the center of the sphere is
Torque about bottom point: \( F \times 2r = I\alpha \)
\( 49 \times 2r = \frac{7}{5}mr^2\alpha \) \( 14 - 4r\alpha \)
As sphere rolls without slipping \( a = r\alpha \) \( a = \frac{14}{4} = \frac{7}{2} = 3.5 m/s^2 \)
Let \( T_r \) be the \( r^{\text{th}} \) term of an A.P. If for some \( m \), \( T_m = \dfrac{1}{25} \), \( T_{25} = \dfrac{1}{20} \), and \( \displaystyle\sum_{r=1}^{25} T_r = 13 \), then \( 5m \displaystyle\sum_{r=m}^{2m} T_r \) is equal to: