/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 15 You wish to make \(a\) round tri... [FREE SOLUTION] | 91Ó°ÊÓ

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You wish to make \(a\) round trip from Earth in a spaceship, traveling at constant speed in a straight line for 6 months on your watch and then returning at the same constant speed. You wish, further, to find Earth to be 1000 years older on your return. (a) What is the value of your constant speed with respect to Earth? (b) How much do you age during the trip? (c) Does it matter whether or not you travel in a straight line? For example, could you travel in a huge circle that loops back to Earth?

Short Answer

Expert verified
(a) The speed is close to the speed of light, specifically \( v \approx c - \frac{c}{2000000} \). (b) You age 1 year during the trip. (c) The path shape (straight line or circle) does not matter, the key is the speed and duration.

Step by step solution

01

- Understanding the time dilation formula

Time dilation is described by the formula: \ \ \[ t' = \frac{t}{\sqrt{1 - \left( \frac{v^2}{c^2} \right)}} \] where: \ \ \( t' \) is the time experienced on Earth, \( t \) is the time experienced on the spaceship, \( v \) is the velocity of the spaceship, \( c \) is the speed of light.
02

- Establish known variables

For Earth, \( t' = 1000 \) years. \ For the spaceship, \( t = 1 \) year (since 6 months out and 6 months back).
03

- Rearrange the time dilation formula to solve for velocity

Rearrange the time dilation formula to solve for \( v \): \ \ \[ v = c \sqrt{1 - \left( \frac{t^2}{t'^2} \right)} \]
04

- Substitute the known values into the formula

Substitute \( t = 1 \) year and \( t' = 1000 \) years : \ \ \[ v = c \sqrt{1 - \left( \frac{1^2}{1000^2} \right)} \] \ \[ v = c \sqrt{1 - \frac{1}{1000000} } \] \ \[ v = c \sqrt{\frac{999999}{1000000}} \]
05

- Simplify the equation

Simplify \[ v = c \left( \sqrt{ \frac{999999}{1000000}}\right) \] \ This simplifies to: \[ v \approx c \left( 1 - \frac{1}{2000000} \right) \]
06

- Calculate the speed

Approximate the speed in terms of c (speed of light): \ \( v \approx c - \frac{c}{2000000} \)
07

- Calculate aging factor for spaceship

According to the original condition, the spaceship travels for 1 year. Thus, the aging will be 1 year.
08

- Analyze the path effect

For part (c), regardless of whether the path is a straight line or a huge circle, the same time dilation principle applies as long as the speed and time duration are consistent, hence it doesn't matter.

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Key Concepts

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

special relativity
Special relativity is a theory proposed by Albert Einstein that describes the physics of objects moving at a constant speed, particularly those moving close to the speed of light. It introduces the idea that the laws of physics are the same for all observers that are moving at a constant velocity relative to each other.
One key outcome of this theory is that time is not absolute. Instead, the time experienced by an observer depends on their relative velocity. This effect is known as time dilation, where a moving clock ticks slower compared to a stationary one. This phenomenon becomes significant at speeds approaching the speed of light.
Special relativity reshapes our understanding of time and space. It highlights that measurements of time intervals and distances can vary based on an observer's motion, leading us to perceive time and space as intertwined in a four-dimensional spacetime fabric.
Lorentz transformation
The Lorentz transformation equations are fundamental to special relativity. They describe how measurements of time and space by two observers in uniform relative motion are related.
When an object moves close to the speed of light, its time and space coordinates need to be transformed between observers. The Lorentz transformation formulas are:
\( t' = \frac{t - \frac{vx}{c^2}}{\frac{1}{\beta}} \) \ \( x' = (x - vt) \beta \)
where:
  • \( t \) is the time in the stationary frame
  • \( t' \) is the time in the moving frame
  • \( x \) is the position in the stationary frame
  • \( x' \) is the position in the moving frame
  • \( v \) is the relative velocity between the two frames
  • \( c \) is the speed of light
  • \( \beta = \frac{1}{\frac{1}{\beta}} \)

These transformations ensure that the speed of light remains constant in all reference frames, a cornerstone of special relativity.
constant velocity
In physics, constant velocity means that an object is moving in a straight line without changing its speed. In the context of special relativity, maintaining a constant velocity is crucial because the principles and equations of special relativity, such as the Lorentz transformations and time dilation, specifically apply to objects moving at constant speeds.
When we say a spaceship is traveling at a constant velocity, it means it doesn't accelerate or decelerate. This simplifies the analysis as we don't need to account for changes in momentum or energy that come with speeding up or slowing down.
Constant velocity ensures that the observed relativistic effects, such as time dilation, are predictable and consistent throughout the journey. This concept is crucial for understanding how time and space behave under special relativity.
relativistic effects
Relativistic effects become significant as an object's speed approaches the speed of light. One of the most striking relativistic effects is time dilation. This means that to an observer on Earth, time on a fast-moving spaceship appears to slow down. For instance, if you travel in a spaceship close to the speed of light, you would age much more slowly than someone on Earth.
Another effect is length contraction, where the length of an object moving at relativistic speeds appears shorter in the direction of motion from the viewpoint of a stationary observer.
These effects are described by the Lorentz transformation and are confirmed by numerous experiments. For high-speed particles in accelerators, their lifetimes appear longer than particles at rest due to time dilation. Similarly, global positioning systems (GPS) need to account for these relativistic effects to provide accurate location data.
Understanding relativistic effects helps in comprehending the behavior of objects in high-speed travel and reinforces the groundbreaking implications of Einstein's special relativity.

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Most popular questions from this chapter

A flash of light is emitted at an angle \(\phi^{\prime}\) with respect to the \(x^{\prime}\) axis of the rocket frame. (a) Show that the angle \(\phi\) the direction of motion of this flash makes with respect to the \(x\) axis of the laboratory frame is given by the equation $$ \cos \phi=\frac{\cos \phi^{\prime}+v^{\mathrm{rel}} / c}{1+\left(v^{\mathrm{rel}} / c\right) \cos \phi^{\prime}} . $$ Optional: Show that your answer to Problem 34 gives the same result when the velocity \(v^{\prime}\) is given the value \(c .\) (b) A light source at rest in the rocket frame emits light uniformly in all directions. In the rocket frame \(50 \%\) of this light goes into the forward hemisphere of a sphere surrounding the source. Show that in the laboratory frame this \(50 \%\) of the light is concentrated in a narrow forward cone of half-angle \(\phi_{0}\) whose axis lies along the direction of motion of the particle. Derive the following expression for the halfangle \(\phi_{0}\) : $$ \cos \phi_{0}=v^{\mathrm{rel}} / c $$ This result is called the headlight effect. (c) What is the half-angle \(\phi_{0}\) in degrees for a light source moving at \(99 \%\) of the speed of light?

An unpowered spaceship whose rest length is 350 meters has a speed \(0.82 c\) with respect to Earth. A micrometeorite, also with speed of \(0.82 c\) with respect to Earth, passes the spaceship on an antiparallel track that is moving in the opposite direction. How long does it take the micrometeorite to pass the spaceship as measured on the ship?

Identical experiments are carried out (1) in a high-speed train moving at constant speed along a horizontal track with the shades drawn and \((2)\) in a closed freight container on the platform as the train passes. Copy the following list and mark with a "yes" quantities that will necessarily be the same as measured in the two frames. Mark with a "no" quantities that are not necessarily the same as measured in the two frames. (a) The time it takes for light to travel one meter in a vacuum; (b) the kinetic energy of an electron accelerated from rest through a voltage difference of one million volts; (c) the time for half the number of radioactive particles at rest to decay; (d) the mass of a proton; (e) the structure of DNA for an amoeba; (f) Newton's Second Law of Motion: \(F=m a ;(\mathrm{g})\) the value of the downward acceleration of gravity \(g\).

A particle moves with speed \(v^{\prime}\) in the \(x^{\prime} y^{\prime}\) plane of the rocket frame and in a direction that makes an angle \(\phi^{\prime}\) with the \(x^{\prime}\) axis. Find the angle \(\phi\) that the velocity vector of this particle makes with the \(x\) axis of the laboratory frame. (Hint: Transform space and time displacements rather than velocities.)

A spaceship of rest length \(100 \mathrm{~m}\) passes a laboratory timing station in \(0.2\) microseconds measured on the timing station clock. (a) What is the speed of the spaceship in the laboratory frame? (b) What is the Lorentz-contracted length of the spaceship in the laboratory frame?

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