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A particle moves along the \(x\) " axis of frame \(S^{\prime}\) with velocity \(0.40 \mathrm{c}\). Frame \(S^{\prime}\) moves with velocity \(0.60 \mathrm{c}\) with respect to frame \(S .\) What is the velocity of the particle with respect to frame \(S ?\)

Short Answer

Expert verified
The velocity of the particle with respect to frame \( S \) is approximately \( 0.806c \).

Step by step solution

01

Identify Given Information

We have two velocities given: the velocity of the particle in frame \( S' \), which is \( v_{p'} = 0.40c \), and the velocity of frame \( S' \) with respect to \( S \), which is \( v_{S'} = 0.60c \). Here, \( c \) is the speed of light.
02

Use the Velocity Addition Formula

We need to find the velocity of the particle relative to frame \( S \) using the relativistic velocity addition formula: \( v = \frac{v_{p'} + v_{S'}}{1 + \frac{v_{p'} v_{S'}}{c^2}} \). This formula accounts for the effects of special relativity when adding velocities.
03

Plug in the Values

Substitute \( v_{p'} = 0.40c \) and \( v_{S'} = 0.60c \) into the formula: \[ v = \frac{0.40c + 0.60c}{1 + \frac{0.40c \times 0.60c}{c^2}}.\] Simplify to get \[ v = \frac{1.00c}{1 + 0.24}.\]
04

Simplify the Equation

Calculate the denominator: \( 1 + 0.24 = 1.24 \). Then, divide the numerator by the denominator: \[ v = \frac{1.00c}{1.24}.\]
05

Compute the Final Velocity

Perform the division to find \( v \): \[ v \approx 0.806c.\] Thus, the velocity of the particle with respect to frame \( S \) is approximately \( 0.806c \).

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Key Concepts

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

special relativity
The theory of special relativity, proposed by Albert Einstein in 1905, revolutionized our understanding of physics by introducing ideas of space and time being interconnected. Before special relativity, it was assumed that the laws of physics were identical for all frames of reference moving at constant speeds relative to each other. However, special relativity extended this principle to include scenarios involving near-light speeds.

This groundbreaking theory introduced two major postulates:
  • The laws of physics are invariant in all inertial frames of reference (i.e., non-accelerating frames).
  • The speed of light in a vacuum is the same for all observers, regardless of the motion of light source or observer.
These postulates laid the foundation for understanding phenomena such as time dilation and length contraction, which occur when objects move at significant fractions of the speed of light, greatly affecting our observations in different reference frames.
velocity in different reference frames
In the realm of special relativity, velocities are not simply additive as they are in classical physics. Instead, we must consider the relativistic velocity addition formula. This formula helps us calculate the velocity of an object as observed from a different reference frame. This consideration becomes particularly important when dealing with objects moving at speeds close to that of light.

The relativistic velocity addition formula is given by:\[v = \frac{v_{1} + v_{2}}{1 + \frac{v_{1} v_{2}}{c^2}}\]where:
  • \(v\) is the resultant velocity observed in the new reference frame.
  • \(v_{1} \) and \(v_{2} \) are the velocities that are being added.
  • \(c\) is the constant speed of light.
The formula accounts for relativistic effects, ensuring no resultant velocity exceeds the speed of light, which is consistent with the principles of special relativity.
speed of light
The speed of light, denoted as \(c\), is fundamental to special relativity and is one of the most important constants in physics. Light travels at approximately \(3 \times 10^8\) meters per second (or about 299,792 kilometers per second) in a vacuum. This speed is exceedingly fast compared to everyday speeds and is considered the ultimate speed limit in the universe.

Several crucial aspects of the speed of light make it unique:
  • It remains constant across all inertial frames, serving as a universal benchmark for comparing velocities.
  • It is independent of the motion of the source or observer, an idea that radically shifts the classical understanding of speed.
  • It sets a limitation where no information or matter can travel faster than light, ensuring causality is preserved in the universe.
These attributes of the speed of light significantly impact our understanding of time, space, and energy, forming a cornerstone of modern physics.

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Most popular questions from this chapter

The car-in-the-garage problem. Carman has just purchased the world's longest stretch limo, which has a proper length of \(L_{c}=30.5 \mathrm{~m} .\) In Fig. \(37-32 a,\) it is shown parked in front of a garage with a proper length of \(L_{g}=6.00 \mathrm{~m}\). The garage has a front door (shown open) and a back door (shown closed). The limo is obviously longer than the garage. Still, Garageman, who owns the garage and knows something about relativistic length contraction, makes a bet with Carman that the limo can fit in the garage with both doors closed. Carman, who dropped his physics course before reaching special relativity, says such a thing, even in principle, is impossible. To analyze Garageman's scheme, an \(x_{c}\) axis is attached to the limo, with \(x_{c}=0\) at the rear bumper, and an \(x_{k}\) axis is attached to the garage, with \(x_{g}=0\) at the (now open) front door. Then Carman is to drive the limo directly toward the front door at a velocity of \(0.9980 c\) (which is, of course, both technically and financially impossible). Carman is stationary in the \(x_{c}\) reference frame; Garageman is stationary in the \(x_{z}\) reference frame. There are two events to consider. Event 1 : When the rear bumper clears the front door, the front door is closed. Let the time of this event be zero to both Carman and Garageman: \(t_{\mathrm{s} 1}=t_{c 1}=0\). The event occurs at \(x_{c}=x_{g}=0 .\) Figure \(37-32 b\) shows event 1 according to the \(x_{g}\) reference frame. Event 2 : When the front bumper reaches the back door, that door opens. Figure \(37-32 c\) shows event 2 according to the \(x_{g}\) reference frame. According to Garageman, (a) what is the length of the limo, and what are the spacetime coordinates (b) \(x_{R 2}\) and (c) \(t_{g 2}\) of event \(2 ?\) (d) For how long is the limo temporarily "trapped" inside the garage with both doors shut? Now consider the situation from the \(x_{c}\) reference frame, in which the garage comes racing past the limo at a velocity of \(-0.9980 \mathrm{c}\). According to Carman, (e) what is the length of the passing garage, what are the spacetime coordinates (f) \(x_{c 2}\) and \((g) t_{c 2}\) of event \(2,(h)\) is the limo ever in the garage with both doors shut, and (i) which event occurs first? (j) Sketch events 1 and 2 as seen by Carman. (k) Are the events causally related; that is, does one of them cause the other? (I) Finally, who wins the bet?

A garden hose with an internal diameter of \(1.9 \mathrm{~cm}\) is connected to a (stationary) lawn sprinkler that consists merely of a container with 24 holes, each \(0.13 \mathrm{~cm}\) in diameter. If the water in the hose has a speed of \(0.91 \mathrm{~m} / \mathrm{s},\) at what speed does it leave the sprinkler holes?

A certain particle of mass \(m\) has momentum of magnitude \(m c .\) What are (a) \(\beta,(b) \gamma,\) and \((c)\) the ratio \(K / E_{0} ?\)

What is the speed parameter for the following speeds: (a) a typical rate of continental drift ( 1 in \(/ y\) ); (b) a typical drift speed for electrons in a current-carrying conductor \((0.5 \mathrm{~mm} / \mathrm{s}) ;\) (c) a highway speed limit of \(55 \mathrm{mi} / \mathrm{h} ;\) (d) the root-mean-square speed of a hydrogen molccule at room temperature; (c) a supersonic plane flying at Mach \(2.5(1200 \mathrm{~km} / \mathrm{h}) ;\) (f) the escape speed of a projectile from the Earth's surface; (g) the speed of Earth in its orbit around the Sun; (h) a typical recession speed of a distant quasar due to the cosmological expansion \(\left(3.0 \times 10^{4} \mathrm{~km} / \mathrm{s}\right) ?\)

A spaceship approaches Earth at a speed of \(0.42 c .\) A light on the front of the ship appears red (wavelength \(650 \mathrm{nm}\) ) to passengers on the ship. What (a) wavelength and (b) color (blue, green, or yellow) would it appear to an observer on Earth?

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