To determine the ratio of the squares of the speeds \(v_1^2\) and \(v_2^2\), we examine the dynamics of a solid sphere rolling without slipping down an inclined plane. The speed at the base is derived from the conservation of energy, specifically the conversion of potential energy to kinetic energy. The formula for the speed at the bottom is:
\(v = \sqrt{\frac{10gh}{7}}\)
Here, \(g\) represents the acceleration due to gravity, and \(h\) is the vertical height of the incline. The height \(h\) can be expressed in terms of the incline's length \(L\) and angle \(\theta\) as:
\(h = L \sin \theta\)
Substituting this into the velocity equation yields:
\(v = \sqrt{\frac{10gL \sin \theta}{7}}\)
Consider two distinct scenarios:
To find the ratio \(v_1^2 : v_2^2\), we square these velocities:
The resulting ratio is:
\(v_1^2 : v_2^2 = \frac{5gL/7}{5\sqrt{2}gL/7} = 1 : \sqrt{2}\)
This result, \(1 : \sqrt{2}\), aligns with the provided correct answer.
An object of uniform density rolls up the curved path with the initial velocity $v_o$ as shown in the figure. If the maximum height attained by an object is $\frac{7v_o^2}{10 g}$ ($g=$ acceleration due to gravity), the object is a _______

A uniform rod of mass m and length l suspended by means of two identical inextensible light strings as shown in figure. Tension in one string immediately after the other string is cut, is _______ (g = acceleration due to gravity). 