Given:
Step 1: Calculate the Frictional Force
The kinetic friction force is given by:
\[ f_k = \mu_k \times N \]
Since the normal force \( N \) is equal to the weight of the body:
\[ N = mg = 10 \times 9.8 = 98 \text{ N} \]
\[ f_k = 0.5 \times 98 = 49 \text{ N} \]
Step 2: Apply Newton's Second Law
The net force acting on the body is:
\[ F_{ ext{net}} = F - f_k \]
\[ F_{ ext{net}} = 60 - 49 = 11 \text{ N} \]
Now, using Newton's second law:
\[ F = ma \]
\[ 11 = 10a \]
\[ a = \frac{11}{10} = 1.1 \approx 1 \text{ m/s}^2 \]
Answer: The acceleration of the body is about 1 m/s² (Option D).
To solve this problem, we first calculate the frictional force acting on the body. The frictional force \( f_{\text{friction}} \) is given by: \[ f_{\text{friction}} = \mu \cdot N \] where: - \( \mu = 0.5 \) is the coefficient of kinetic friction, - \( N = m \cdot g \) is the normal force, and \( m = 10 \, \text{kg} \), \( g = 9.8 \, \text{ms}^{-2} \). Thus, \[ N = 10 \times 9.8 = 98 \, \text{N} \] Now calculate the frictional force: \[ f_{\text{friction}} = 0.5 \times 98 = 49 \, \text{N} \] The net force \( F_{\text{net}} \) acting on the body is the applied force minus the frictional force: \[ F_{\text{net}} = F_{\text{applied}} - f_{\text{friction}} = 60 \, \text{N} - 49 \, \text{N} = 11 \, \text{N} \] The resulting acceleration \( a \) can be found using Newton's second law: \[ F_{\text{net}} = m \cdot a \] \[ a = \frac{F_{\text{net}}}{m} = \frac{11}{10} = 1 \, \text{ms}^{-2} \]
Thus, the resulting acceleration is \( 1 \, \text{ms}^{-2} \), and the correct answer is (D).
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 
Match List-I with List-II and select the correct option: 