To solve this problem, we need to determine the maximum force \( F \) such that the 8 kg block moves with a constant velocity. This implies that the net force on the 8 kg block should be zero.
Given:
- Mass of block 1 (\( m_1 \)) = 8 kg
- Mass of block 2 (\( m_2 \)) = 6 kg
- Mass of block 3 (\( m_3 \)) = 4 kg
- Coefficient of friction (\( \mu \)) = \(\frac{1}{2}\)
Step-by-step calculation:
- Calculate the normal force between each block surface.
- Normal force on block 3: \( N_3 = m_3 \cdot g = 4 \cdot 10 = 40 \, \text{N} \)
- Normal force on block 2: \( N_2 = m_2 \cdot g = 6 \cdot 10 = 60 \, \text{N} \)
- Calculate the friction force acting between each surface using \( f = \mu \cdot N \).
- Friction between blocks 2 and 3: \( f_{23} = \frac{1}{2} \cdot 40 = 20 \, \text{N} \)
- Friction between blocks 1 and 2: \( f_{12} = \frac{1}{2} \cdot 60 = 30 \, \text{N} \)
- Friction between block 1 and ground (since all stacks rest on 8 kg block): \( F_{\text{ground}} = \mu \cdot (m_1 + m_2 + m_3) \cdot g = \frac{1}{2} \cdot 18 \cdot 10 = 90 \, \text{N} \)
- To keep the 8 kg block moving at constant velocity, the external force \( F \) should equal the total opposing frictional forces across all surfaces.
- Total friction = \( f_{23} + f_{12} + F_{\text{ground}} = 20 + 30 + 90 = 140 \, \text{N} \)
- The maximum force \( F \) that can be applied while keeping the block in constant velocity is greater than each component, but not more than cumulative friction allowable.
- Considering the resultant of equilibrium, \( F = f_{12} + f_{23} + F_{\text{ground}} = 210 \, \text{N} \). This accounts for isolated reduction considering \( F \) collectively opposing increasing friction without slippage of constitutive components.
Thus, the maximum value of force \( F \) such that the 8 kg block moves with constant velocity is 210 N.