
To solve this problem, we need to calculate the forces \(|\vec{F_1}|\) and \(|\vec{F_2}|\), and then find the difference \(|\vec{F_1}| - |\vec{F_2}|\).
Given:
The forces 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 limiting friction is given by:
\(F_{\text{friction}} = \mu \cdot F_{\text{gravity perpendicular}} = \mu \cdot mg \cos(\theta)\)
To move the block up, apply enough force to overcome both gravity and friction:
\(|\vec{F_1}| = F_{\text{gravity parallel}} + F_{\text{friction}}\)
\(= mg \sin(\theta) + \mu mg \cos(\theta)\)
Substituting values:
\(|\vec{F_1}| = 5 \cdot 10 \cdot \sin(30^\circ) + 0.1 \cdot 5 \cdot 10 \cdot \cos(30^\circ)\)
\(= 50 \cdot 0.5 + 0.1 \cdot 50 \cdot \frac{\sqrt{3}}{2}\)
\(= 25 + 2.5\sqrt{3}\)
To prevent sliding down, counteract gravity by friction:
\(|\vec{F_2}| = F_{\text{gravity parallel}} - F_{\text{friction}}\)
\(= mg \sin(\theta) - \mu mg \cos(\theta)\)
Substituting values:
\(|\vec{F_2}| = 5 \cdot 10 \cdot \sin(30^\circ) - 0.1 \cdot 5 \cdot 10 \cdot \cos(30^\circ)\)
\(= 25 - 2.5\sqrt{3}\)
\(|\vec{F_1}| - |\vec{F_2}| = (25 + 2.5\sqrt{3}) - (25 - 2.5\sqrt{3})\)
\(= 5\sqrt{3} \, \text{N}\)
Thus, the correct answer is \(5\sqrt{3} \, \text{N}\).
The block experiences frictional force due to the roughness of the inclined surface. The kinetic friction force \( f_k \) is given by:
\[ f_k = \mu mg \cos \theta, \]where \( \mu = 0.1 \) is the coefficient of friction, \( m = 5 \, \text{kg} \), and \( \theta = 30^\circ \).
Calculating \( f_k \):
\[ f_k = 0.1 \times 5 \times 10 \times \cos 30^\circ = 0.1 \times 50 \times \frac{\sqrt{3}}{2} = 2.5 \sqrt{3} \, \text{N}. \]To move the block up the incline, the force \( F_1 \) must overcome both the component of gravitational force along the incline and the frictional force. Therefore:
\[ F_1 = mg \sin \theta + f_k. \]Substitute the values:
\[ F_1 = 5 \times 10 \times \sin 30^\circ + 2.5 \sqrt{3} = 25 + 2.5 \sqrt{3} \, \text{N}. \]To prevent the block from sliding down, the force \( F_2 \) must balance the component of gravitational force along the incline, reduced by the frictional force. Thus:
\[ F_2 = mg \sin \theta - f_k. \]Substitute the values:
\[ F_2 = 25 - 2.5 \sqrt{3} \, \text{N}. \]The difference \( |F_1 - F_2| \) is:
\[ |F_1 - F_2| = |(25 + 2.5 \sqrt{3}) - (25 - 2.5 \sqrt{3})| = 5 \sqrt{3} \, \text{N}. \]Thus, the answer is:
\[ 5 \sqrt{3} \, \text{N}. \]A sphere of radius R is cut from a larger solid sphere of radius 2R as shown in the figure. The ratio of the moment of inertia of the smaller sphere to that of the rest part of the sphere about the Y-axis is : 
A, B and C are disc, solid sphere and spherical shell respectively with the same radii and masses. These masses are placed as shown in the figure. 
The moment of inertia of the given system about PQ is $ \frac{x}{15} I $, where $ I $ is the moment of inertia of the disc about its diameter. The value of $ x $ is:
If $ \theta \in [-2\pi,\ 2\pi] $, then the number of solutions of $$ 2\sqrt{2} \cos^2\theta + (2 - \sqrt{6}) \cos\theta - \sqrt{3} = 0 $$ is:
A thin transparent film with refractive index 1.4 is held on a circular ring of radius 1.8 cm. The fluid in the film evaporates such that transmission through the film at wavelength 560 nm goes to a minimum every 12 seconds. Assuming that the film is flat on its two sides, the rate of evaporation is: