
To solve this problem, we need to analyze the forces acting on the system where a horizontal force \( F \) is applied at the midpoint of the rope, causing it to make a \( 45^\circ \) angle with the vertical. The setup is shown in the image above.
\(T_1 \cos(45^\circ) = mg\)
Given, \( m = 1 \, \text{kg} \) and \( g = 10 \, \text{m/s}^2 \). Thus:
\(T_1 \times \frac{1}{\sqrt{2}} = 1 \times 10\)
\(T_1 = 10 \sqrt{2} \, \text{N}\)
\(T_1 \sin(45^\circ) = F\)
Substituting the value of \( T_1 \):
\(10 \sqrt{2} \times \frac{1}{\sqrt{2}} = F\)
\(F = 10 \, \text{N}\)
Hence, the correct answer is \( 10 \, \text{N} \).
We are given that a mass of 1 kg is suspended by a rope, and a horizontal force F is applied at the midpoint of the rope, making an angle of 45° with the vertical.
Let \( T_1 \) be the tension in the rope at the point of application of the force and \( T_2 \) be the tension in the vertical section of the rope.
From \( T_1 \cos 45^\circ = T_2 \), we have:
\[ T_1 \cos 45^\circ = 10 \, \text{N}. \]
Since \( \cos 45^\circ = \frac{1}{\sqrt{2}} \), we find:
\[ T_1 \times \frac{1}{\sqrt{2}} = 10 \quad \implies \quad T_1 = 10\sqrt{2}. \]
Now, substituting into the equation \( T_1 \sin 45^\circ = F \):
\[ 10\sqrt{2} \times \frac{1}{\sqrt{2}} = F \quad \implies \quad F = 10 \, \text{N}. \]
Thus, the magnitude of the force is 10 N, and the correct answer is Option (4).
Two blocks of masses \( m \) and \( M \), \( (M > m) \), are placed on a frictionless table as shown in figure. A massless spring with spring constant \( k \) is attached with the lower block. If the system is slightly displaced and released then \( \mu = \) coefficient of friction between the two blocks.
(A) The time period of small oscillation of the two blocks is \( T = 2\pi \sqrt{\dfrac{(m + M)}{k}} \)
(B) The acceleration of the blocks is \( a = \dfrac{kx}{M + m} \)
(\( x = \) displacement of the blocks from the mean position)
(C) The magnitude of the frictional force on the upper block is \( \dfrac{m\mu |x|}{M + m} \)
(D) The maximum amplitude of the upper block, if it does not slip, is \( \dfrac{\mu (M + m) g}{k} \)
(E) Maximum frictional force can be \( \mu (M + m) g \)
Choose the correct answer from the options given below:
A wooden block of mass M lies on a rough floor. Another wooden block of the same mass is hanging from the point O through strings as shown in the figure. To achieve equilibrium, the coefficient of static friction between the block on the floor and the floor itself is 
Let \( C_{t-1} = 28, C_t = 56 \) and \( C_{t+1} = 70 \). Let \( A(4 \cos t, 4 \sin t), B(2 \sin t, -2 \cos t) \text{ and } C(3r - n_1, r^2 - n - 1) \) be the vertices of a triangle ABC, where \( t \) is a parameter. If \( (3x - 1)^2 + (3y)^2 = \alpha \) is the locus of the centroid of triangle ABC, then \( \alpha \) equals: