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An electron of \(\beta=0.999987\) moves along the axis of an evacuated tube that has a length of \(5.00 \mathrm{~m}\) as measured by a laboratory observer \(S\) at rest relative to the tube. An observer \(S^{\prime}\) who is at rest relative to the electron, however, would see this tube moving with speed \(v(=\beta c)\). What length would observer \(S^{\prime}\) measure for the tube?

Short Answer

Expert verified
Observer \(S^\prime\) measures a contracted length substantially less than 5 m due to the high speed of the electron.

Step by step solution

01

Understanding the Scenario

We are given that an electron is moving at a significant fraction of the speed of light (indicated by \(\beta = 0.999987\)), along an evacuated tube 5 meters long. Observer \(S\), at rest relative to the tube, measures this length. Observer \(S^\prime\), moving with the electron, measures the tube's length as it moves past them.
02

Identify the Formula for Length Contraction

We need to apply the concept of length contraction from the theory of relativity. The length of an object in motion, as measured by an observer at rest relative to the object, appears contracted. The formula for calculating the contracted length \(L'\) is: \[ L' = L \sqrt{1 - \beta^2} \]where \(L\) is the proper length (5 meters in this case), and \(\beta\) is the object's velocity expressed as a fraction of the speed of light.
03

Calculate \(\beta^2\)

Given \(\beta = 0.999987\), we calculate \(\beta^2\) as follows: \[ \beta^2 = (0.999987)^2 \]This will result in a value that we will use in the next step to find \(\sqrt{1 - \beta^2}\).
04

Calculate the Length Contraction Factor

Compute \(1 - \beta^2\):\[ 1 - \beta^2 = 1 - (0.999987)^2 \]Find the square root of this difference to determine the contraction factor:\[ \sqrt{1 - \beta^2} \]Moving forward, this value will help us calculate the contracted length \(L'\).
05

Compute the Contracted Length \(L'\)

Using the contraction formula and the values found so far, compute the contracted length \(L'\).\[ L' = 5 \times \sqrt{1 - \beta^2} \]Substitute the value of \(\sqrt{1 - \beta^2}\) calculated in the previous step.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Length Contraction
Length contraction is an intriguing consequence of the theory of relativity. It describes how the observed length of an object in motion appears shortened (or contracted) to an observer in a different inertial frame of reference.
This phenomenon occurs because, as objects travel at a significant fraction of the speed of light, they exhibit different measurements of space along their direction of motion. For length contraction:
  • The proper length, denoted as \(L\), is the length of the object measured by an observer at rest relative to it.
  • The contracted length, \(L'\), is the length measured by an observer moving relative to the object.
To find the contracted length \(L'\), we use the formula:\[L' = L \sqrt{1 - \beta^2}\]Here, \(\beta = \frac{v}{c}\), representing the object's velocity as a fraction of the speed of light \(c\).
This adjustment makes lengths appear shorter for fast-moving objects from the perspective of a stationary observer.
Theory of Relativity
The theory of relativity encompasses two key components: special relativity and general relativity. Proposed by Albert Einstein in the early 20th century, these theories revolutionized the way we understand space, time, and motion. In our context, we focus on special relativity.
Special relativity primarily deals with objects moving at constant speeds close to the speed of light. Its fundamental principles include:
  • The laws of physics are the same for all observers in uniform motion relative to each other.
  • The speed of light in a vacuum is constant and does not change regardless of the motion of the source or observer.
A unique outcome of these principles is the relativistic effects, such as time dilation and length contraction, which arise due to the invariance of the speed of light.
Special Relativity
Special relativity focuses on the behavior of objects moving at high velocities and introduces groundbreaking ideas about the fabric of space and time. It suggests that time and space are not absolute; instead, they are intertwined in a four-dimensional spacetime continuum.
Within this framework, key concepts include:
  • Time dilation: As objects move closer to the speed of light, time experienced by these objects slows down relative to a stationary observer.
  • Length contraction: Fast-moving objects appear shorter in the direction of motion, as viewed from a stationary frame of reference.
These effects occur because the universe demands the speed of light remain constant, leading to the transformation of space and time measurements between different inertial frames. Special relativity shifts our intuition of how objects behave as they near light speed, drastically changing our perception of distance and time.
Motion of Electrons
In the context of special relativity, electrons behaving at high speeds, like in the given exercise, illustrate the practical effects of relativistic physics. Electrons moving close to the speed of light experience length contraction, affecting how observers measure dimensions like the length of a tube.
When electrons travel at such high velocities:
  • They exhibit relativistic mass, meaning their mass effectively increases, requiring more energy to speed up.
  • Observations of their motion provide insights into high-energy particle physics and technologies, such as accelerators used in scientific research.
  • Understanding these dynamics allows scientists to predict behaviors in various fields, including electronics and quantum mechanics.
The study of electrons at near-light speeds helps validate the predictions of special relativity, reaffirming the theory's applicability to microscopic and macroscopic scales.

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Most popular questions from this chapter

(Come) back to the future. Suppose that a father is \(25.0 \mathrm{y}\) older than his daughter. He wants to travel outward from Earth for \(2.000 \mathrm{y}\) and then back for another \(2.000 \mathrm{y}\) (both intervals as he measures them) such that he is then \(25.0\) y younger than his daughter. What constant speed parameter \(\beta\) (relative to Earth) is required?

A spaceship, moving away from Earth at a speed of \(0.850 c\), reports back by transmitting at a frequency (measured in the spaceship frame) of \(100 \mathrm{MHz}\). To what frequency must Earth receivers be tuned to receive the report?

A spaceship is moving away from Earth at speed \(0.333 c\). A source on the rear of the ship emits light at wavelength \(450 \mathrm{~nm}\) according to someone on the ship. What (a) wavelength and (b) color (blue, green, yellow, or red) are detected by someone on Earth watching the ship?

An unstable high-energy particle enters a detector and leaves a track of length \(0.856 \mathrm{~mm}\) before it decays. Its speed relative to the detector was \(0.992 c\). What is its proper lifetime? That is, how long would the particle have lasted before decay had it been at rest with respect to the detector?

Bullwinkle in reference frame \(S^{\prime}\) passes you in reference frame \(S\) along the common direction of the \(x^{\prime}\) and \(x\) axes, as in Fig. 37-9. He carries three meter sticks: meter stick 1 is parallel to the \(x^{\prime}\) axis, meter stick 2 is parallel to the \(y^{\prime}\) axis, and meter stick 3 is parallel to the \(z^{\prime}\) axis. On his wristwatch he counts off \(10.0 \mathrm{~s}\), which takes \(30.0 \mathrm{~s}\) according to you. Two events occur during his passage. According to you, event 1 occurs at \(x_{1}=33.0 \mathrm{~m}\) and \(t_{1}=22.0 \mathrm{~ns}\), and event 2 occurs at \(x_{2}=53.0 \mathrm{~m}\) and \(t_{2}=62.0 \mathrm{~ns} .\) According to your measurements, what is the length of (a) meter stick 1, (b) meter stick 2, and (c) meter stick 3? According to Bullwinkle, what are \((\mathrm{d})\) the spatial separation and \((\mathrm{e})\) the temporal separation between events 1 and 2 , and (f) which event occurs first?

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