We have two masses, \( m_1 = 1.5 \, \text{kg} \) and \( m_2 = 2 \, \text{kg} \), connected by a light rope on a frictionless horizontal surface. We need to find the maximum force that can be applied to the second mass without breaking the rope, which can withstand a maximum tension of 60 N. We will also consider the case where the rope has a mass of 0.1 kg.
First, consider the system where the rope is massless. The maximum tension the rope can handle is 60 N. When a force \( F \) is applied to the second mass, the tension in the rope will be equal to the force required to accelerate the first mass \( m_1 \).
Using Newton's second law for \( m_1 \):
\[
T = m_1 \cdot a
\]
where \( T = 60 \, \text{N} \) is the maximum tension and \( a \) is the acceleration of the system.
The total mass of the system is \( m_1 + m_2 = 1.5 \, \text{kg} + 2 \, \text{kg} = 3.5 \, \text{kg} \).
Using Newton's second law for the entire system:
\[
F = (m_1 + m_2) \cdot a
\]
Substituting \( a = \frac{T}{m_1} \) into the equation for \( F \):
\[
F = (m_1 + m_2) \cdot \frac{T}{m_1}
\]
Substitute the known values:
\[
F = (3.5) \cdot \frac{60}{1.5} = 140 \, \text{N}
\]
Now, consider the rope has a mass of 0.1 kg. The total mass of the system becomes \( m_1 + m_2 + m_{\text{rope}} = 3.6 \, \text{kg} \).
The tension in the rope will still be 60 N, but now the acceleration \( a \) is given by:
\[
a = \frac{T}{m_1 + \frac{m_{\text{rope}}}{2}}
\]
The force \( F \) applied to the system is:
\[
F = (m_1 + m_2 + m_{\text{rope}}) \cdot a
\]
Substitute the known values:
\[
a = \frac{60}{1.5 + \frac{0.1}{2}} = \frac{60}{1.55} \approx 38.7097 \, \text{m/s}^2
\]
\[
F = 3.6 \cdot 38.7097 \approx 139.355 \, \text{N}
\]
- Maximum force without rope mass: \(\boxed{140 \, \text{N}}\)
- Maximum force with rope mass: \(\boxed{139.355 \, \text{N}}\)