/*! 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 29 A rod lies parallel to the \(x\)... [FREE SOLUTION] | 91Ó°ÊÓ

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A rod lies parallel to the \(x\) axis of reference frame \(S\), moving along this axis at a speed of \(0.892 c\). Its rest length is \(1.70 \mathrm{~m}\). What will be its measured length in frame \(S ?\)

Short Answer

Expert verified
The length of the rod in frame \(S\) is approximately 0.768 meters.

Step by step solution

01

Understand Lorentz Contraction

The length of an object moving at a high velocity will be different from its rest length due to the effects of special relativity. This phenomenon is known as Lorentz contraction. The formula for Lorentz contraction is given by \[ L = L_0 \sqrt{1 - \frac{v^2}{c^2}} \] where \(L_0\) is the rest length of the object, \(L\) is the length measured in the moving frame, \(v\) is the velocity of the object, and \(c\) is the speed of light.
02

Identify Given Values

In this problem, the rest length \(L_0\) of the rod is given as \(1.70\) meters. The velocity \(v\) of the rod relative to frame \(S\) is \(0.892c\), where \(c\) is the speed of light.
03

Substitute Values into Lorentz Contraction Formula

Substitute the given values into the Lorentz contraction formula:\[ L = 1.70 \sqrt{1 - \frac{(0.892c)^2}{c^2}} \] which simplifies to \[ L = 1.70 \sqrt{1 - 0.892^2} \]
04

Calculate the Square of Velocity Fraction

Calculate the square of \(0.892\):\[ 0.892^2 = 0.795664 \]
05

Compute the Lorentz Factor

Now, calculate the Lorentz factor:\[ \sqrt{1 - 0.795664} = \sqrt{0.204336} \approx 0.451986 \]
06

Calculate the Contracted Length

Finally, use the Lorentz factor to find the length in frame \(S\):\[ L = 1.70 \times 0.451986 \approx 0.768 \text{ meters} \]
07

Conclusion: Measured Length in Frame S

The length of the rod as measured in frame \(S\) will be approximately \(0.768\) meters.

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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 in physics formulated by Albert Einstein, that revolutionized our understanding of space and time. It describes how objects behave when they move at high speeds, close to the speed of light. One of the key postulates of Special Relativity is that the laws of physics are the same in all inertial reference frames, meaning no reference frame is more special than any other. Another crucial aspect of the theory is that the speed of light in a vacuum is constant and does not depend on the motion of the light source or observer.

This fundamentally changes how we perceive measurements of time and space for objects in motion. Unlike our everyday intuition, which is based on Newtonian physics, Special Relativity shows us that time and space are intertwined into what is known as spacetime.
  • This leads to phenomena such as time dilation, where time appears to move slower for a moving observer compared to a stationary one.
  • Another important consequence is length contraction, which we will delve into shortly.
Overall, Special Relativity helps us understand how the universe operates at speeds approaching the speed of light, challenging and expanding our previous conceptions of space and time.
Length Contraction
Length contraction is a fascinating outcome of Special Relativity, occurring when an object is moving close to the speed of light compared to an observer. As the object's speed increases, its length along the direction of motion appears shorter to the observer. This contraction is only noticeable when the speeds involved are significant fractions of the speed of light, denoted by the constant \(c\).

The phenomenon is mathematically described by the Lorentz Contraction formula:
  • The formula is \( L = L_0 \sqrt{1 - \frac{v^2}{c^2}} \), where \(L_0\) is the object's rest length, \(v\) is its velocity, and \(L\) is the measured contracted length.
For example, if a rod of rest length \(1.70\) meters is moving at \(0.892c\), its length from a stationary frame is shorter, around \(0.768\) meters.

The closer the speed is to \(c\), the more dramatic the contraction, illustrating the non-linear nature of the space and time relationship in relativistic physics. Length contraction does not occur in the direction perpendicular to the motion, highlighting that this effect is direction-dependent.
Speed of Light
The speed of light in a vacuum is approximately \(299,792,458\) meters per second, commonly denoted as \(c\). It is one of the fundamental constants of nature and plays a vital role in the theory of Special Relativity. According to Einstein's postulate, the speed of light is the ultimate speed limit in our universe. Nothing can surpass this speed.

Light's speed being constant in all inertial frames introduces several counterintuitive effects, such as time dilation and length contraction. These effects are not noticeable in everyday experiences since they are only significant at velocities close to \(c\).
  • No matter how fast you are moving or in what direction, light will always seem to move at \(c\) from your reference frame.
  • This uniformity leads to the relativity of simultaneity, where two events happening simultaneously in one frame may not be simultaneous in another.
Understanding the speed of light and its constancy is essential for grasping the principles and predictions of Special Relativity.
Reference Frames
In the context of physics, a reference frame is a perspective or a viewpoint from which measurements like time, position, and velocity are made. Inertial reference frames are those where objects are either at rest or move at constant velocity. In these frames, the laws of physics hold uniformly, as postulated by Special Relativity.

When discussing concepts like length contraction, it’s crucial to consider the reference frames involved. Length contraction is observed in the reference frame in which the object is moving. At rest, the observer's frame is different, and they would measure the object at its full rest length.
  • The concept emphasizes how different observers can perceive motion differently based on their respective frames.
  • Motion relative to each frame can affect measurements of both time and space.
The use of reference frames helps us understand and predict how different observers, even if moving relative to each other, can consistently describe physical phenomena. Adaptation to different reference frames is one of the key skills in dealing with relativistic problems.

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