/*! 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 53 Sara Settlemyer is an intelligen... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

Sara Settlemyer is an intelligent layperson who carefully reads articles about science in the public press. She has the objections to relativity listed below. Respond to each of Sara's objections clearly, decisively, and politely- without criticizing her! (a) "Observer A says that observer B's clock runs slow, while \(\mathrm{B}\) says that A's clock runs slow. This is a logical contradiction. Therefore relativity should be abandoned." (b) "Observer A says that B's meter sticks are contracted along their direction of relative motion. B says that A's meter sticks are contracted. This is a logical contradiction. Therefore relativity should be abandoned." (c) "Anybody with common sense knows that travel at high speed in the direction of a receding light pulse decreases the speed with which the pulse recedes. Hence a flash of light cannot have the same speed for observers in relative motion. With this disproof of the Principle of Relativity, all of relativity collapses." (d) "Relativity is preoccupied with how we observe things, not with what is really happening. Therefore relativity is not a scientific theory, since science deals with reality." (e) "Relativity offers no way to describe an event without coordinates, and no way to speak about coordinates without referring to one or another particular reference frame. However, physical events have an existence independent of all choice of coordinates and reference frames. Therefore the special relativity you talk about in this chapter cannot be the most fundamental theory of events and the relation between events."

Short Answer

Expert verified
Relativity is consistent within its framework of relative motion, postulates the invariance of light speed, and uses coordinates to describe but not define physical events.

Step by step solution

01

Addressing Clock Contradiction (a)

Explain that in relativity, time dilation is an observed effect depending on the relative motion between observers. It's not a contradiction because each observer measures the other's clock running slow due to their relative motion, as predicted by the theory. This symmetry is a fundamental part of relativity and does not imply a logical flaw.
02

Addressing Meter Stick Contraction (b)

Describe that length contraction, like time dilation, is also relative. When Observer A measures B's meter sticks and finds them contracted, B will measure A's meter sticks and find the same contraction. This phenomenon arises from the principles of relativity and is consistent, not contradictory.
03

Speed of Light and Relative Motion (c)

Point out that one of the core postulates of relativity is that the speed of light is constant for all observers, regardless of their relative motion. This means even if an observer moves towards or away from the light pulse, the speed of light remains unchanged, preserving the consistency of the theory.
04

Scientific Focus of Relativity (d)

Clarify that relativity indeed deals with observations because how we measure and observe phenomena is fundamental in understanding physical laws. However, these observations are reflective of the underlying physical reality and thus are very much within the scope of science.
05

Coordinates and Reference Frames (e)

Explain that while relativity uses coordinates and reference frames for description, these are tools for understanding the physical laws that govern events. The independence of physical events from coordinates reaffirms the robustness of relativity rather than undermining it, as it shows the phenomena exist independently of how we choose to describe them.

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with 91Ó°ÊÓ!

Key Concepts

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

Time Dilation
Time dilation is a fascinating consequence of Einstein's theory of relativity. It means that time can pass at different rates for different observers, depending on their relative motion. When Observer A sees Observer B's clock running slow, it's not a contradiction. In fact, B will also see A's clock running slow. Both observations are correct because time itself stretches or contracts depending on the speed at which the observers are moving relative to each other.
For example, if A is traveling in a fast spaceship, and B is on Earth, each will see the other's clock ticking slower. This happens because the speed of light is the same for everyone, and to keep that consistent, time has to adjust. This concept helps explain why time dilation is not a logical flaw but a fundamental aspect of our universe accepted by scientists.
Length Contraction
Length contraction is another interesting part of relativity. Just like time, lengths also change depending on the relative motion between observers. Observer A will see Observer B's meter sticks as shorter. Similarly, B will see A's meter sticks as shorter too.
Imagine A and B are both in spaceships traveling at a high speed past each other. Each will see the other's spaceship as contracted, or shorter, in the direction of motion. This isn't a contradiction but a predicted outcome of moving at significant fractions of the speed of light. It's an understandable and real effect that happens because the universe works to keep the speed of light constant for everyone.
Constant Speed of Light
One of the most remarkable aspects of relativity is that the speed of light is always constant, regardless of how fast an observer is moving. Whether you're moving towards the light source or away from it, the speed of light stays the same.
This can seem strange because, with most everyday objects, the speed does change. For instance, if you walk against a moving train, the speed of the train appears slower relative to you. However, light doesn't behave this way. This constancy of the speed of light forms the backbone of relativity and helps scientists understand how time and space adjust to maintain this constant speed.
Observer Reference Frames
In relativity, the concept of reference frames is critical. It matters where the observer is and how they are moving compared to what they are observing. The laws of physics are the same in every reference frame, but the measurements of time, length, and other quantities can look different.
For example, if two observers are moving relative to each other, they will have different experiences of time and space. The idea that physical events happen independently of how we describe them shows the consistency of relativity. Observing how things change makes us understand more deeply the principles governing these changes.
Scientific Theory Validity
The validity of relativity as a scientific theory lies in its ability to describe real phenomena accurately and predict outcomes reliably. Science often deals with observations because that's how we learn about the underlying reality. While relativity might seem to focus on observations, it actually reveals much about how the universe functions.
Relativity is tested and confirmed through numerous experiments and observations. It gives us a powerful framework to understand the universe, even if we can't see its effects with our naked eyes every day. By validating its predictions through experiments, relativity remains a cornerstone of modern physics.

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

A meter stick lies at rest in the rocket frame and makes an angle \(\phi^{\prime}\) with the \(x^{\prime}\) axis as measured by the rocket observer. The laboratory observer measures the \(x\) - and \(y\) -components of the meter stick as it streaks past. From these components the laboratory observer computes the angle \(\phi\) that the stick makes with his \(x\) axis. (a) Find an expression for the angle \(\phi\) in terms of the angle \(\phi^{\prime}\) and the relative speed \(v^{\text {rel }}\) between rocket and laboratory frames. (b) What is the length of the "meter" stick measured by the laboratory observer? (c) Optional: Why is your expression in part (a) different from equations derived in Problems 34 and \(35 ?\)

(a) Find an equation for the unknown mass \(m\) of a particle if you know its momentum \(p\) and its kinetic energy \(K\). Show that this expression reduces to an expected result for nonrelativistic particle speeds. (b) Find the mass of a particle whose kinetic energy is \(K=55.0 \mathrm{MeV}\) and whose momentum is \(p=\) \(121 \mathrm{MeV} / \mathrm{c}\). Express your answer as a decimal fraction or multiple of the mass \(m_{\mathrm{e}}\) of the electron.

Galaxy A is measured to be receding from us on Earth with a speed of \(0.3 c .\) Galaxy \(\mathrm{B}\), located in precisely the opposite direction, is also receding from us at the same speed. What recessional velocity will an observer on galaxy A measure (a) for our galaxy, and (b) for galaxy B?

A pulse of protons arrives at detector \(\mathrm{D}\), where you are standing. Prior to this, the pulse passed through detector C, which lies 60 meters upstream. Detector C sent a light flash in your direction at the same instant that the pulse passed through it. At detector D you receive the light flash and the proton pulse separated by a time of 2 nanoseconds \(\left(2 \times 10^{-9} \mathrm{~s}\right)\). What is the speed of the proton pulse?

A gamma ray (an energetic photon) falls on a nucleus of initial mass \(m\), initially at rest. The energy \(E_{\mathrm{p}}\) of the incoming gamma ray matches the energy separation between the lowest energy of the nucleus and its first excited state, so the incident photon is absorbed. We want to know the mass \(m^{*}\) of the excited nucleus. (see Fig. \(38-13 .\) ) (a) Show that the conservation of energy and momentum equations are, in an obvious notation: and $$ \begin{array}{c} E_{\mathrm{p}}+m c^{2}=E_{m^{*}} \\ \frac{E_{\mathrm{p}}}{c}=p_{m^{*}}=\frac{\left(E_{m^{*}}^{2}-m^{* 2} c^{4}\right)^{1 / 2}}{c} . \end{array} $$ (b) Combine the two conservation equations to find an expression for \(m^{*}\) as a function of \(E_{\mathrm{p}}, m\), and \(c\). (c) Show that for very small values of \(E_{\mathrm{p}}\) the limiting result is \(m^{*}=m .\) Explain why this limiting result is reasonable.

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.