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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?

Short Answer

Expert verified
Speed: \(5 \times 10^8 \text{ m/s}\), Lorentz-contracted length: \(36 \text{ m}\)

Step by step solution

01

- Identify Given Data

Rest length of spaceship, \( L_0 = 100 \text{ m} \). Time taken to pass the laboratory, \( t = 0.2 \text{ microseconds} = 0.2 \times 10^{-6} \text{ s} \).
02

- Calculate Speed

The speed of the spaceship in the laboratory frame can be calculated using the formula \( v = \frac{L_0}{t} \). Substituting the given values: \[ v = \frac{100}{0.2 \times 10^{-6}} = 5 \times 10^8 \text{ m/s} \].
03

- Lorentz Contraction Formula

The Lorentz-contracted length \( L \) can be calculated using the formula: \[ L = \frac{L_0}{\beta} \], where \( \beta = \frac{1}{\text{Lorentz factor}} \) and the Lorentz factor is given by \[ \text{Lorentz factor} = \frac{1}{\frac{v^2}{c^2}} \].
04

- Calculate Lorentz Factor

First, compute the Lorentz factor with \( v = 5 \times 10^8 \text{ m/s} \) and the speed of light \( c = 3 \times 10^8 \text{ m/s} \): \[ \text{Lorentz factor} = \frac{1}{\frac{(5 \times 10^8)^2}{(3 \times 10^8)^2}} = \frac{1}{\frac{25 \times 10^{16}}{9 \times 10^{16}}} = \frac{1}{\frac{25}{9}} = \frac{9}{25} \]
05

- Calculate Lorentz-Contraction Length

Since we have \( L = L_0 \times \frac{9}{25} \): Substituting \( L_0 = 100 \text{ m} \), we get \[ L = 100 \times \frac{9}{25} = 36 \text{ m} \].

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Key Concepts

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

Relativistic Speeds
Relativistic speeds are speeds that are a significant fraction of the speed of light. When objects move at these high velocities, classical physics equations no longer apply, and we must turn to Einstein's theory of special relativity. At such speeds, physical quantities like time, length, and mass are affected. To give an idea, if a spaceship moves at 80% of the speed of light, its behavior and perception will be drastically different from what Newtonian physics predicts.
In the given exercise, a spaceship moves at a speed calculated to be \(5 \times 10^8 \text{ m/s}\), well beyond half of the speed of light, which is \(3 \times 10^8 \text{ m/s}\).
This high velocity leads to significant relativistic effects like time dilation and Lorentz contraction.
Time Dilation
Time dilation is a phenomenon predicted by the theory of special relativity. It states that time passes at different rates for observers who are in relative motion to each other. The faster one moves, the slower time ticks for them in comparison to a stationary observer.
Using the exercise as an example, observers on the spaceship would experience time passing more slowly compared to those in the laboratory frame. This difference isn't noticeable at everyday speeds but becomes significant at relativistic speeds. To quantify, time dilation can be calculated using the Lorentz factor, given by \( \gamma = \frac{1}{\sqrt{1 - \frac{v^2}{c^2}}} \).
At the spaceship's speed \(v = 5 \times 10^8 \text{ m/s}\), and with \(c = 3 \times 10^8 \text{ m/s}\), the time for the spaceship occupants slows down markedly, showcasing the intriguing effects of relativistic travel.
Special Relativity
Special relativity is the branch of physics introduced by Albert Einstein in 1905. It revolutionized our understanding of space, time, and energy. The theory is based on two key postulates:
  • The laws of physics are the same in all inertial frames of reference.
  • The speed of light in a vacuum is constant and independent of the motion of all observers.
From these postulates, conclusions about time dilation, length contraction, and the equivalence of mass and energy (\(E = mc^2\)) arise.
In the context of the spaceship problem, special relativity helps us understand how and why the length of the spaceship contracts when viewed from the laboratory frame. The contracted length, calculated using the Lorentz transformation, confirms special relativity's predictions: such effects are not just theoretical but have real, measurable impacts at high velocities.
Thus, through this groundbreaking theory, we can better comprehend the peculiar but fascinating nature of objects traveling close to light speed.

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Most popular questions from this chapter

An aspirin tablet contains 5 grains of aspirin (medicinal unit), which is equal to \(325 \mathrm{mg}\). For how many kilometers would the energy equivalent of this mass power an automobile? Assume \(12.75 \mathrm{~km} / \mathrm{L}\) and a heat of combustion of \(3.65 \times 10^{7} \mathrm{~J} / \mathrm{L}\) for the gasoline used in the automobile.

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?

Through what voltage must an electron be accelerated from rest in order to increase its energy to \(101 \%\) of its rest energy?

Evelvn Brown does not approve of our latticework of rods and clocks and the use of a light flash to synchronize them. (a) "I can synchronize my clocks in any way I choose!" she exclaims. Is she right? (b) Evelyn wants to synchronize two identical clocks, called Big Ben and Little Ben, which are at rest with respect to one another and separated by one million kilometers in their rest frame. She uses a third clock, identical in construction with the first two, that travels with constant velocity between them. As her moving clock passes Big Ben, it is set to read the same time as Big Ben. When the moving clock passes Little Ben, that outpost clock is set to read the same time as the traveling clock. "Now Big Ben and Little Ben are synchronized," says Evelyn Brown. Is Evelyn's method correct? (c) After Evelyn completes her synchronization of Little Ben by her method, how does the reading of Little Ben compare with the reading of a nearby clock on a latticework at rest with respect to Big Ben (and Little Ben) and synchronized by our standard method using a light flash? Evaluate in milliseconds any difference between the reading on Little Ben and the nearby lattice clock in the case that Evelyn's traveling clock moved at a constant velocity of 500000 kilometers per hour from Big Ben to Little Ben. (d) Evaluate the difference in the reading between the EvelynBrown- synchronized Little Ben and the nearby lattice clock when Evelyn's synchronizing traveling clock moves 1000 times as fast as the speed given in part (c).

You are taking a trip from the solar system to our nearest visible neighbor, Alpha Centauri, approximately 4 light-years distant. At launch you experienced a period of acceleration that increased your speed with respect to Earth from zero to nearly half the speed of light. Now your spaceship is coasting in unpowered flight. Compare and contrast the observations you make now with those you made before the rocket took off from the Earth's surface. Be as specific and detailed as possible. Distinguish between observations made inside the cabin with the windows covered and those made looking out of uncovered windows at the front, side, and back of the cabin.

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