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Large Rockets. Suppose we built a rocket that worked much like the Space Shuttle but was 1000 times as large. Could this rocket get us to speeds close to the speed of light? Explain.

Short Answer

Expert verified
No, current physics and technology prevent reaching near-light speeds by simply increasing rocket size.

Step by step solution

01

Understanding the Problem

Our task is to determine if a hypothetical rocket, which is 1000 times larger than the Space Shuttle, could achieve speeds near the speed of light. We need to analyze the physics of rocket propulsion and energy requirements for reaching such speeds.
02

Gravitational and Energy Considerations

To reach speeds near the speed of light, we need to consider the relativistic effects described by Einstein's theory of relativity. As objects near the speed of light, their mass effectively increases, requiring exponentially more energy to continue accelerating. The energy needed is given by \( E = mc^2 \gamma - mc^2 \), where \( \gamma = \frac{1}{\sqrt{1-v^2/c^2}} \).
03

Rocket Propulsion and Fuel Considerations

Rocket propulsion relies on ejecting mass (fuel) to generate thrust. Even if the rocket is 1000 times larger, the amount of fuel required to reach relativistic speeds would be enormous, possibly exceeding the mass of the rocket itself. Furthermore, the speed of ejected fuel limits the achievable velocity, often significantly lower than light speed.
04

Conclusion from Physics Principles

Despite the rocket's increased size, the energy requirements and current propulsion technology constraints make it unfeasible to achieve speeds close to the speed of light. The limitations of mass increase and fuel constraints prevent such acceleration under current scientific understanding.

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Key Concepts

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

Space Shuttle
The Space Shuttle is a marvel of modern engineering and physics, designed to transport astronauts and cargo to space. It operates using rocket propulsion, where fuel is burned and gases are expelled at high speeds out of the shuttle's engines.
This action generates thrust, pushing the shuttle upwards into space, a principle explained by Newton's third law: for every action, there's an equal and opposite reaction. The Shuttle was iconic due to its reusable design, being the first ever aircraft capable of orbiting the Earth, coming back, and then re-flying.
  • It linked the bridge between traditional space capsules and the dream of a future with reusable spacecraft.
  • Each launch was a spectacle of human ingenuity, requiring massive amounts of fuel and forces to overcome Earth's gravity.
Even though its operations were impressive, they weren't without limits. These limitations become evident when considering scaling shuttles to immense sizes or achieving light-speed velocities.
With our current technology, taking a Space Shuttle and making it 1000 times larger would increase fuel and engineering challenges vastly, rather than proportionally.
Relativistic Effects
Relativistic effects become absolutely crucial when dealing with high-speed travel, particularly as objects approach the speed of light. These effects are derived from Einstein's Theory of Relativity, and they are not observable at the low speeds experienced in everyday life.
However, at high velocities, strange phenomena arise, such as length contraction, time dilation, and mass increase.
  • Time Dilation: As velocity approaches light speed, time appears to move slower for the object compared to an outside observer.
  • Length Contraction: Objects appear to contract along the direction of motion when viewed by a stationary observer.
  • Mass Increase: An object's mass effectively increases, making further acceleration incredibly energy demanding.
This mass increase is paramount as it makes reaching light speeds practically impossible with current technology. The closer you get to the speed of light, the more energy is required exponentially, making such speeds unfeasible for a massive object like a Space Shuttle.
Energy Requirements
When considering the energy required to propel a spacecraft to relativistic speeds, the math becomes daunting. Traditional rockets, like the Space Shuttle, utilize chemical fuel, which has its energy limits. As an object moves faster, the energy needed for additional increments of speed increases drastically.
Using Einstein’s formula for relativistic energy, the calculation shows exponential requirements: \[ E = mc^2 \gamma - mc^2 \] where \( \gamma = \frac{1}{\sqrt{1-v^2/c^2}} \).
This indicates that as a rocket approaches light speed, the energy needed diverges to infinity—making it practically impossible to sustain. Even with scaled-up rockets, chemical propulsion can't meet the required energy output.
  • Exponential Energy Growth: The closer the speed of the rocket to light, the more energy is needed exponentially.
  • Resource Limits: Fuel and energy consumption can vastly exceed practical constraints.
Given current technology and resources, achieving such speeds is beyond our scientific and engineering capabilities.
Einstein's Theory of Relativity
Einstein's Theory of Relativity fundamentally transformed our understanding of space, time, and energy. It introduced concepts that defy common intuitive interpretation, fundamentally altering how we perceive motion and speed at high velocities.
The famous equation, \( E = mc^2 \), demonstrates the relationship between mass and energy, emphasizing how energy is required to move mass at increasing speeds, ultimately reaching unattainable levels near light speed. His theory proposed that as speed increases:
  • Energy and mass are equivalent and can be converted into each other.
  • Nothing can exceed the speed of light within a vacuum due to these energy constraints.
This theory is essential when considering high-speed travel. It explains why a massive rocket, even if immensely large, cannot approach light speed as the energy required becomes insurmountable. As we aim for advanced propulsion possibilities, understanding and harnessing these relativistic effects will be crucial.

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Most popular questions from this chapter

Briefly discuss how Einstein's general theory of relativity might allow "shortcuts" by which we could reach distant stars in shorter times than we would expect from their measured distances. Do we know whether these shortcuts are really possible?

Choose the best answer to each of the following. Explain your reasoning with one or more complete sentences. What does the famous formula \(E=m c^{2}\) have to do with special relativity? (a) Nothing; it comes from a different theory. (b) It is one of the two starting assumptions of special relativity. (c) It is a direct consequence of the theory, and hence a way of testing the theory's validity.

What known problems were solved when Einstein discovered the special theory of relativity?

Be sure to show all calculations clearly and state your final answers in complete sentences. The Coral Model of Colonization. We can estimate the time it would take for a civilization to colonize the galaxy. Imagine that a civilization sends colonists to stars that are an average distance \(D\) away and sends them in spacecraft that travel at speed \(v\). The time required for travel, \(t_{\text {ravel }}\), is then \(t_{\text {travel }}=D / v\) Suppose that the colonists build up their colony for a time \(t_{\mathrm{col}}\) at which point they send out their own set of colonists to other star systems (with the same average distance and same spacecraft speed). Then the speed at which the civilization expands outward from the home star, \(v_{\mathrm{col}}\) (for the speed of colonization), is \(v_{\mathrm{col}}=D /\left(t_{\text {travel }}+t_{\mathrm{col}}\right) .\) However, this is true only if the colonization is always directed straight outward from the home star. In reality, the colonists will sometimes go to uncolonized star systems in other directions, so we will introduce a constant \(k\) that accounts for this zigzag motion. Our equation for the speed at which the civilization expands outward from the home star is $$\begin{aligned} v &=k \frac{D}{\left(t_{\text {travel }}+t_{\text {col }}\right)} \\ &=k \frac{D}{\left(\frac{D}{v}+t_{\text {col }}\right)} \end{aligned}$$ For the purposes of this problem, assume that \(k=\frac{1}{2}\) and that the average distance between star systems is \(D=5\) light-years. a. How fast (as a fraction of the speed of light) does the civilization expand if its spacecraft travel at \(0.1 c\) and each colony builds itself up for 150 years before sending out the next wave of colonists? How long would it take the colonists to expand a distance of 100,000 light-years from their home star at this rate? b. Repeat part (a), but assume that the spacecraft travel at \(0.01 c\) and that each colony builds itself up for 1000 years before sending out more colonists. c. Repeat part (a), but assume that the spacecraft travel at \(0.25 c\) and that each colony builds itself up for 50 years before sending out more colonists.

The amount of energy that would be needed to accelerate a large spaceship to a speed close to the speed of light is (a) about 100 times as much energy as is needed to launch the Space Shuttle; (b) more than the total amount of energy used by the entire world in a year; (c) more than the amount of energy that our Sun emits into space in a year.The rocket engines of our current spacecraft are powered by (a) chemical energy; (b) nuclear energy; (c) matter-antimatter annihilation.

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