To solve this problem, we need to analyze the system involving the block, the spring, and the pulley. We can use principles from physics, particularly energy conservation, to find the speed of the block after it falls 1 meter. Let's break it down step by step.
Understanding the System
We have a block of mass \( m = 4 \, \text{kg} \) attached to a spring with a spring constant \( k = 32 \, \text{N/m} \). The pulley has a mass of \( 8 \, \text{kg} \) and can be treated as a disc. Initially, the spring is unstretched, and the system starts from rest.
Key Concepts
- Potential Energy (PE): When the block falls, it loses gravitational potential energy.
- Kinetic Energy (KE): The block gains kinetic energy as it falls.
- Spring Potential Energy: The spring stores energy when it is stretched.
Energy Conservation Principle
We can apply the conservation of mechanical energy, which states that the total mechanical energy in a closed system remains constant if only conservative forces are acting. In this case, we consider the gravitational potential energy, the kinetic energy of the block, and the potential energy stored in the spring.
Initial Energy
Initially, the system has gravitational potential energy due to the height of the block. The initial potential energy (PE_initial) when the block is at rest at height \( h = 1 \, \text{m} \) is given by:
PE_initial = mgh = 4 \, \text{kg} \times 9.81 \, \text{m/s}^2 \times 1 \, \text{m} = 39.24 \, \text{J}
Final Energy
After the block falls 1 meter, it has converted some of its potential energy into kinetic energy (KE) and some into spring potential energy (PE_spring). The final energy (E_final) can be expressed as:
E_final = KE + PE_spring
Where:
- KE = \( \frac{1}{2} mv^2 \)
- PE_spring = \( \frac{1}{2} k x^2 \) (where \( x \) is the stretch of the spring, which is equal to the distance fallen, \( x = 1 \, \text{m} \))
Calculating the Spring Potential Energy
Substituting the values into the spring potential energy formula:
PE_spring = \( \frac{1}{2} \times 32 \, \text{N/m} \times (1 \, \text{m})^2 = 16 \, \text{J} \)
Setting Up the Energy Equation
Now we can set up the energy conservation equation:
PE_initial = KE + PE_spring
39.24 \, \text{J} = \( \frac{1}{2} \times 4 \, \text{kg} \times v^2 + 16 \, \text{J} \)
Solving for Speed
Rearranging the equation to solve for \( v \):
39.24 \, \text{J} - 16 \, \text{J} = \( \frac{1}{2} \times 4 \, \text{kg} \times v^2 \)
23.24 \, \text{J} = \( 2 \, \text{kg} \times v^2 \)
v^2 = \( \frac{23.24 \, \text{J}}{2 \, \text{kg}} = 11.62 \, \text{m}^2/\text{s}^2 \)
v = \( \sqrt{11.62} \approx 3.41 \, \text{m/s} \)
Final Result
Therefore, the speed of the block after it falls 1 meter is approximately \( 3.41 \, \text{m/s} \). This calculation illustrates how energy is transformed from potential to kinetic and elastic forms in a mechanical system. Understanding these principles is crucial in physics, as they apply to many real-world scenarios.