An annular disk of mass π, inner radius π and outer radius π is placed on a horizontal surface with coefficient of friction π, as shown in the figure. At some time, an impulse β0π₯Μ is applied at a height β above the center of the disk. If β = βπ then the disk rolls without slipping along the π₯-axis.Which of the following statement(s) is(are) correct?
(1) For π β 0 and π β 0, \(β_π = \frac{π}{2}\). This statement suggests that when the coefficient of friction is nonzero and the inner radius (a) tends to 0, the height (βπ) at which the impulse is applied is equal to half the outer radius(\(\frac{b}{2}\)). This statement is correct. When the inner radius approaches 0, the entire disk participates in the rolling motion, and the height at which the impulse is applied becomes equal to half the outer radius. Therefore, this option is correct.
(2) For π β 0 and π β π, βπ = π. This statement suggests that when the coefficient of friction is nonzero and the inner radius (a) tends to the outer radius (b), the height (βπ) at which the impulse is applied is equal to the outer radius (b). This statement is correct. When the inner radius approaches the outer radius, the entire disk participates in the rolling motion, and the height at which the impulse is applied becomes equal to the outer radius. Therefore, this option is correct.
(3) For β = βπ, the initial angular velocity does not depend on the inner radius a. This statement is correct. The initial angular velocity of the disk does not depend on the inner radius a. The initial angular velocity is determined by the impulse applied and the moment of inertia of the disk. The inner radius does not affect these factors. Therefore, this option is correct.
(4) For π = 0 and β = 0, the wheel always slides without rolling. This statement is correct. When the coefficient of friction is zero and the impulse is applied at the same height as the center of mass (β = 0), the wheel will slide without rolling. In this case, there is no friction force to initiate rolling motion, so the wheel will simply slide. Therefore, this option is correct.
Therefore correct statements are (A), (B), (C) and (D)
The moment of inertia πΌcmβ of a ring-shaped disc, with an inner radius πa, an outer radius b, and a mass m, about an axis perpendicular to the disc and passing through its center C, is given by:
\(πΌ_{cm}=\frac{1}{π}(π^2+π^2)\)
where π2 and π2 are the squares of the inner and outer radii, respectively.
The linear impulse π½πβ changes the linear momentum of the disc. Right after the impulse is applied, the linear momentum can be represented as:
ππ£cm=π½πβ
where m is the mass of the disc and vcmβ is the velocity of the center of mass resulting from the impulse.
The angular impulse about the center of mass C of the disc is applied in a clockwise direction, with its magnitude being π½π,ang=βπ½πβ. These impulse changes the angular momentum of the disc about point C, expressed as:
πΌcmπ=π½π,ang=βπ½πβ
where Icmβ is the moment of inertia of the disc about its center of mass, Ο is the angular velocity resulting from the angular impulse, Joβ is the linear impulse, and h is a factor relating the angular impulse to the linear impulse.
For the disc to roll without slipping, given that the friction coefficient ΞΌ is non-zero, the condition is π£cm=ππ. By substituting the expressions for π£cmβ and Ο and solving, we obtain the following relationship for the minimum value of h (denoted as hmβ):
\(h_m \frac{I_{\text{cm}}}{m_b} = \frac{a^2 + b^2}{26}\)
where πΌcmβ is the moment of inertia of the disc about its center of mass, m is the mass of the disc, a is the inner radius, and b is the outer radius of the disc.
By substituting π=0 into the formula, we find that \(h_m = \frac{1}{2}\)This implies that a solid disc will roll without slipping if the impulse is applied midway along the upper half of the disc.
Similarly, substituting π=π yields βπ=π. This indicates that a ring (an annular disc with equal inner and outer radii) will roll without slipping when the horizontal impulse is applied at the very top of the ring.
For the condition where β=βπβ, the initial angular velocity Ο is given by:
\(\omega = \frac{h_mJ_o}{I _ {cm} \, m_b}\)
This expression for the angular velocity is independent of the inner radius a of the disc.
When a wheel is placed on a smooth surface with no friction (ΞΌ=0) and an impulse is applied directly at its center (h=0), there is no torque generated to initiate rotation. Consequently, under these conditions, if an impulse is delivered to the center of a wheel on a frictionless surface, the wheel will invariably slide and not roll.
A tube of length 1m is filled completely with an ideal liquid of mass 2M, and closed at both ends. The tube is rotated uniformly in horizontal plane about one of its ends. If the force exerted by the liquid at the other end is \( F \) and the angular velocity of the tube is \( \omega \), then the value of \( \alpha \) is ______ in SI units.
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
The center of a disk of radius $ r $ and mass $ m $ is attached to a spring of spring constant $ k $, inside a ring of radius $ R>r $ as shown in the figure. The other end of the spring is attached on the periphery of the ring. Both the ring and the disk are in the same vertical plane. The disk can only roll along the inside periphery of the ring, without slipping. The spring can only be stretched or compressed along the periphery of the ring, following Hookeβs law. In equilibrium, the disk is at the bottom of the ring. Assuming small displacement of the disc, the time period of oscillation of center of mass of the disk is written as $ T = \frac{2\pi}{\omega} $. The correct expression for $ \omega $ is ( $ g $ is the acceleration due to gravity): 
Let $ a_0, a_1, ..., a_{23} $ be real numbers such that $$ \left(1 + \frac{2}{5}x \right)^{23} = \sum_{i=0}^{23} a_i x^i $$ for every real number $ x $. Let $ a_r $ be the largest among the numbers $ a_j $ for $ 0 \leq j \leq 23 $. Then the value of $ r $ is ________.
Rotational motion can be defined as the motion of an object around a circular path, in a fixed orbit.
The wheel or rotor of a motor, which appears in rotation motion problems, is a common example of the rotational motion of a rigid body.
Other examples: