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Spaceships of the future may be powered by ion-propulsion engines in which ions are ejected from the back of the ship to drive it forward. In one such engine the ions are to be ejected with a speed of \(0.80 c\) relative to the spaceship. The spaceship is traveling away from the earth at a speed of \(0.70 \mathrm{c}\) relative to the earth. What is the velocity of the ions relative to the earth? Assume that the direction in which the spaceship is traveling is the positive direction, and be sure to assign the correct plus or minus signs to the velocities.

Short Answer

Expert verified
The velocity of the ions relative to Earth is \(-0.227c\).

Step by step solution

01

Identify the Given Values

We are given the following velocities:1. The velocity of the spaceship relative to Earth is \( v_{s} = +0.70c \).2. The velocity of ions relative to the spaceship is \( v_{i/s} = -0.80c \).(Note that it is negative because ions are ejected backwards from the spaceship as it travels forwards.)
02

Apply the Relativistic Velocity Addition Formula

We need to find the velocity of the ions relative to Earth, \( v_{i} \). Use the relativistic velocity addition formula: \[v_{i} = \frac{v_{i/s} + v_{s}}{1 + \frac{v_{i/s}v_{s}}{c^2}}\]
03

Substitute the Values into the Formula

Substitute the given values into the formula:\[v_{i} = \frac{-0.80c + 0.70c}{1 + \frac{(-0.80c)(0.70c)}{c^2}}\]
04

Simplify the Expression

Calculate the numerator and the denominator:\[v_{i} = \frac{-0.10c}{1 - 0.56}\]This simplifies to:\[v_{i} = \frac{-0.10c}{0.44}\]
05

Calculate the Final Velocity

Perform the division to find the velocity of the ions relative to Earth:\[v_{i} = -0.227c\]This means the ions are moving towards Earth at this velocity.

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Key Concepts

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

Ion-Propulsion Engines
Ion-propulsion engines mark a revolutionary leap in space exploration technology. Unlike traditional chemical rockets that burn fuel to generate thrust, ion-propulsion engines operate by accelerating ions using electric fields. This process results in the expulsion of ions at high speeds, propelling the spacecraft forward.

These engines offer several advantages:
  • Greater Efficiency: Ion-propulsion systems are far more efficient than chemical rockets, as they can accelerate particles to speeds of approximately 30-40 kilometers per second.
  • Long Duration Missions: Due to their efficient use of fuel, ion-propulsion systems are ideal for long-duration missions where power conservation is critical.
Ion propulsion is particularly suitable for deep-space missions, where high-speed, long-term thrust is vital. These engines could power spacecraft on long journeys, perhaps to distant planets or other star systems, fundamentally changing human capabilities in space travel.
Special Relativity
Special relativity is a theory proposed by Albert Einstein that revolutionized our understanding of physics, especially applicable when objects move at speeds close to that of light. One of the critical postulates of special relativity is that the speed of light, denoted as \(c\), is a constant and nothing can exceed it.

Relativistic effects become significant at speeds approaching \(c\), such as:
  • Time Dilation: Time appears to slow down for objects moving close to the speed of light, compared to an observer at rest.
  • Length Contraction: Objects in motion are measured to be shorter in the direction of motion by an observer at rest.
  • Relativistic Velocity Addition: The velocities of objects moving at high speeds do not simply add linearly; instead, they combine according to the relativistic velocity addition formula.
Understanding these effects is crucial for accurate calculations in high-speed scenarios, such as those encountered by spacecraft using ion-propulsion engines. As shown in the introductory problem, failing to apply relativistic calculations would lead to incorrect assessments of velocities, impacting mission planning and safety in space missions.
Space Travel Physics
Space travel physics involves understanding the various forces and principles that govern the movement of spacecraft through space. At its core, it considers the fundamental laws of motion, as defined by Newton, alongside modifications introduced by Einstein's theory of relativity.

Key principles include:
  • Newton's Laws of Motion: These provide the foundational understanding for calculating force, acceleration, and the behavior of spacecraft in space.
  • Gravitational Influences: The gravitational fields of planets, stars, and other celestial bodies affect the trajectory and velocity of spacecraft.
  • Relativistic Effects: As space travel often involves high speeds, relativistic effects can influence time, distance, and velocity, requiring precise calculations for long-distance travel.
Incorporating these concepts allows scientists and engineers to design efficient flight paths, optimize fuel usage, and ensure the safe and successful execution of space missions. The interactions between these principles define the possibilities and limitations of modern and future space exploration.

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Most popular questions from this chapter

There are many astonishing consequences of special relativity, two of which are time dilation and length contraction. Problem 50 reviews these important concepts in the context of a golf game in a hypothetical world where the speed of light is only a little faster than that of a golf cart. Other important consequences of special relativity are the equivalence of mass and energy, and the dependence of kinetic energy on the total energy and on the rest energy. Problem 51 serves as a review of the roles played by mass and energy in special relativity. Imagine playing golf in a world where the speed of light is only \(c=3.40 \mathrm{m} / \mathrm{s} .\) Golfer A drives a ball down a flat horizontal fairway for a distance that he measures as \(75.0 \mathrm{m}\). Golfer \(\mathrm{B}\), riding in a cart, happens to pass by just as the ball is hit (see the figure). Golfer A stands at the tee and watches while golfer \(\mathrm{B}\) moves down the fairway toward the ball at a constant speed of \(2.80 \mathrm{m} / \mathrm{s}\). Concepts: (i) Who measures the proper length of the drive, and who measures the contracted length? (ii) Who measures the proper time interval, and who measures the dilated time interval? Calculations: (a) How far is the ball hit according to golfer \(B ?\) (b) According to each golfer, how much time does it take golfer \(\mathrm{B}\) to reach the ball?

A \(6.00-\mathrm{kg}\) object oscillates back and forth at the end of a spring whose spring constant is \(76.0 \mathrm{N} / \mathrm{m}\). An observer is traveling at a speed of \(1.90 \times 10^{8} \mathrm{m} / \mathrm{s}\) relative to the fixed end of the spring. What does this observer measure for the period of oscillation?

Determine the ratio of the relativistic kinetic energy to the nonrelativistic kinetic energy \(\left(\frac{1}{2} m v^{2}\right)\) when a particle has a speed of (a) \(1.00 \times 10^{-3} c\) and (b) \(0.970 c\)

Suppose that you are planning a trip in which a spacecraft is to travel at a constant velocity for exactly six months, as measured by a clock on board the spacecraft, and then return home at the same speed. Upon your return, the people on earth will have advanced exactly one hundred years into the future. According to special relativity, how fast must you travel? Express your answer to five significant figures as a multiple of \(c-\) for example, \(0.95585 \mathrm{c}\)

The rest energy \(E_{0}\) and the total energy \(E\) of three particles, expressed in terms of a basic amount of energy \(E^{\prime}=5.98 \times 10^{-10} \mathrm{J},\) are listed in the table. The speeds of these particles are large, in some cases approaching the speed of light. Concepts: (i) Given the rest energies specified in the table, what is the ranking (largest first) of the masses of the particles? (ii) Is the kinetic energy KE given by the expression \(\mathrm{KE}=1 / 2 m v^{2},\) and what is the ranking (largest first) of the kinetic energies of the particles? Calculations: For each particle, determine its (a) mass and (b) kinetic energy. $$ \begin{array}{ccc} \hline \text { Particle } & \text { Rest Energy } & \text { Total Energy } \\ \hline \mathrm{a} & E^{\prime} & 2 E^{\prime} \\ \mathrm{b} & E^{\prime} & 4 E^{\prime} \\ \mathrm{c} & 5 E^{\prime} & 6 E^{\prime} \\ \hline \end{array} $$

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