Chapter 36: Problem 96
A \(1.88-\mathrm{kg}\) mass oscillates on the end of a spring whose spring stiffness constant is \(k=84.2 \mathrm{~N} / \mathrm{m}\). If this system is in a spaceship moving past Earth at \(0.900 c,\) what is its period of oscillation according to \((a)\) observers on the ship, and (b) observers on Earth?
Short Answer
Step by step solution
Understand the Problem
Determine the Formula in Rest Frame
Calculate the Period for Observer on Ship
Account for Relativistic Effects for Earth Observer
Calculate the Period for Observer on Earth
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Simple Harmonic Motion
In SHM, the main players are displacement, velocity, acceleration, and restoring force. These elements are all tied together in such a way that makes the motion cyclical.
- Displacement refers to how far the object is from its equilibrium position.
- Velocity is the speed at which the object is traveling, while acceleration describes how this speed changes.
- The restoring force is what pulls the object back toward its equilibrium position. In the case of a mass-spring system, this is provided by the spring.
- \( T \) is the period,
- \( m \) is the mass of the object,
- and \( k \) is the spring stiffness constant.
Time Dilation
This might seem strange because we usually think of time as constant. However, in the realm of high velocities, especially near the speed of light, things become more flexible.
- This concept is essential in the context of relativistic physics, where observers in different frames of reference (like on a spaceship versus on Earth) measure different times for the same event.
- For example, in the exercise above, observers on Earth see the spaceship's oscillating mass having a longer period than observers on the spaceship due to time dilation.
- \( T' \) is the dilated period,
- \( T \) is the original period observed from the moving frame,
- \( v \) is the velocity of the moving object,
- and \( c \) is the speed of light.
Mass-Spring System
This system makes a great example to study simple harmonic motion, as the spring provides the returning force needed for oscillation.
- The mass represents the object that moves back and forth.
- The spring provides the restoring force, following Hooke’s Law, which states that the force exerted by a spring is proportional to the displacement of the spring from its equilibrium position: \( F = -kx \), where \( F \) is force, \( k \) is the spring constant, and \( x \) is the displacement.