Chapter 3: Problem 170
The system is at rest with the spring unstretched when \(\theta=0 .\) The 3 -kg particle is then given a slight nudge to the right. \((a)\) If the system comes to momentary rest at \(\theta=40^{\circ},\) determine the spring constant \(k .(b)\) For the value \(k=100 \mathrm{N} / \mathrm{m},\) find the speed of the particle when \(\theta=25^{\circ} .\) Use the value \(b=0.40 \mathrm{m}\) throughout and neglect friction.
Short Answer
Step by step solution
Analyzing Initial Conditions
Energy Conservation Equation
Analyzing the System at \(\theta = 0\)
Analyzing the System at \(\theta = 40^{\circ}\)
Substitute Known Values and Solve for \(k\)
Calculate Component Values for \(\theta = 40^{\circ}\)
Solving for Speed at \(\theta = 25^{\circ}\) with \(k = 100 \text{ N/m}\)
Substitute Values and Solve for Velocity
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Physics Problems
For this type of problem:
- Define initial and final states of the system.
- Identify forces involved, such as gravitational or spring forces.
- Apply relevant equations, like conservation of energy, to find unknown variables.
Spring Mechanics
- The force in a spring: \( F = -kx \)
- \( F \) is the force exerted by the spring,
- \( k \) is the spring constant, and
- \( x \) is the displacement from its equilibrium position.
- \( PE_{spring} = \frac{1}{2} k x^2 \).
Kinetic and Potential Energy
- Kinetic Energy (KE): It's the energy of motion.
- Expressed by the equation:
- \( KE = \frac{1}{2}mv^2 \)
- Where \( m \) is mass, and \( v \) is velocity.
- Potential Energy (PE): Considered stored energy.
- Examples include gravitational and elastic potential energy.
As these energies transform into one another, they help us understand and predict the motion of objects in a system. Whenever an object's energy is not lost to the environment, total energy remains consistent, cycling between kinetic and potential forms.
Energy Conservation Equations
- Equation: \( PE_{gravity} + PE_{spring} + KE = \text{constant} \)
- Start by calculating all forms of energy at different points.
- Seamlessly transition between energy types for solutions.
- Apply this concept to activities ranging from simple pendulums to complex oscillations.