
To resolve this issue, we must compute the magnitudes of forces \(|\vec{F_1}|\) and \(|\vec{F_2}|\) and subsequently determine their difference, \(|\vec{F_1}| - |\vec{F_2}|\).
Provided data:
The forces acting on the block, parallel and perpendicular to the inclined plane, are:
\(F_{\text{gravity parallel}} = mg \sin(\theta)\)
\(F_{\text{gravity perpendicular}} = mg \cos(\theta)\)
The maximum static friction is calculated as:
\(F_{\text{friction}} = \mu \cdot F_{\text{gravity perpendicular}} = \mu \cdot mg \cos(\theta)\)
The force to move the block upwards must counteract both gravitational pull and friction:
\(|\vec{F_1}| = F_{\text{gravity parallel}} + F_{\text{friction}}\)
\(= mg \sin(\theta) + \mu mg \cos(\theta)\)
Substitution of values yields:
\(|\vec{F_1}| = 5 \cdot 10 \cdot \sin(30^\circ) + 0.1 \cdot 5 \cdot 10 \cdot \cos(30^\circ)\)
\(= 50 \cdot 0.5 + 0.1 \cdot 50 \cdot \frac{\sqrt{3}}{2}\)
\(= 25 + 2.5\sqrt{3}\)
To prevent downward motion, the applied force must balance the component of gravity acting down the incline, opposed by friction:
\(|\vec{F_2}| = F_{\text{gravity parallel}} - F_{\text{friction}}\)
\(= mg \sin(\theta) - \mu mg \cos(\theta)\)
Substituting the given values:
\(|\vec{F_2}| = 5 \cdot 10 \cdot \sin(30^\circ) - 0.1 \cdot 5 \cdot 10 \cdot \cos(30^\circ)\)
\(= 25 - 2.5\sqrt{3}\)
\(|\vec{F_1}| - |\vec{F_2}| = (25 + 2.5\sqrt{3}) - (25 - 2.5\sqrt{3})\)
\(= 5\sqrt{3} \, \text{N}\)
Therefore, the final result is \(5\sqrt{3} \, \text{N}\).
A circular disc has radius \( R_1 \) and thickness \( T_1 \). Another circular disc made of the same material has radius \( R_2 \) and thickness \( T_2 \). If the moments of inertia of both the discs are same and \[ \frac{R_1}{R_2} = 2, \quad \text{then} \quad \frac{T_1}{T_2} = \frac{1}{\alpha}. \] The value of \( \alpha \) is __________.
A solid cylinder of radius $\dfrac{R}{3}$ and length $\dfrac{L}{2}$ is removed along the central axis. Find ratio of initial moment of inertia and moment of inertia of removed cylinder. 