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A small rocket burns 0.0500 kg of fuel per second, ejecting it as a gas with a velocity relative to the rocket of magnitude 1600 m/s. (a) What is the thrust of the rocket? (b) Would the rocket operate in outer space where there is no atmosphere? If so, how would you steer it? Could you brake it?

Short Answer

Expert verified
(a) Thrust is 80 N. (b) Yes, it operates in space. Steering is possible by adjusting thrust direction; braking via a retro-burn.

Step by step solution

01

Understand Thrust Formula

Thrust is the force exerted by the rocket's engine as it expels gas. The formula for thrust ( \( F \) ) is given by: \[ F = \dot{m} \cdot v_e \] where \( \dot{m} \) is the mass flow rate of fuel and \( v_e \) is the relative velocity of the exhaust gas.
02

Identify Given Values

From the information given: - The mass flow rate of fuel, \( \dot{m} = 0.0500 \ \text{kg/s} \). - The relative velocity of the exhaust, \( v_e = 1600 \ \text{m/s} \).
03

Calculate the Thrust

Using the thrust formula: \[ F = \dot{m} \cdot v_e \] Substitute the given values: \[ F = 0.0500 \ \text{kg/s} \cdot 1600 \ \text{m/s} = 80 \ \text{N} \] Thus, the thrust of the rocket is 80 N.
04

Determine Rocket Operation in Outer Space

Rockets can operate in outer space because they rely on the expulsion of gases for thrust, not on air around them. The thrust depends solely on the mass flow rate and the velocity of the expelled gas.
05

Exploring Steering and Braking

Steering in space can be achieved by adjusting the direction of the exhaust gas ejection, using fins, gimballed engines, or directional nozzles. Braking can be performed by reversing the thrust direction, for example, by turning the rocket around and firing the engines, which is often referred to as a retro-burn.

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Key Concepts

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

Mass Flow Rate
The mass flow rate is a fundamental concept in rocket propulsion. It represents the amount of mass being expelled from the rocket per unit of time. In simpler terms, it tells us how fast the fuel is being used and turned into exhaust gas.
The mass flow rate has a direct impact on the thrust a rocket can generate. This is because the higher the mass flow rate, the more mass there is to accelerate, thus increasing the force exerted by the rocket. It is typically measured in kilograms per second (kg/s).
  • In our example, the mass flow rate is 0.0500 kg/s.
  • This means that 0.0500 kg of fuel is burnt and ejected as exhaust every second.
An intuitive way to understand this is by comparing it to a garden hose. The more water flows out of the hose per second, the stronger the water pressure felt on your hand.​
Exhaust Velocity
The exhaust velocity is another crucial aspect of rocket propulsion. It indicates the speed at which the exhaust gases are expelled from the rocket. This speed is relative to the rocket itself.
Think of the exhaust velocity as how fast the rocket pushes back against the ejected gases. The faster the gases are expelled, the greater the force on the rocket in the opposite direction. This principle is defined by Newton's third law: for every action, there is an equal and opposite reaction.
  • In the given problem, the exhaust velocity is 1600 m/s.
  • This means the gases are pushed out at a speed of 1600 meters every second.
High exhaust velocity is essential for achieving efficient rocket thrust and is influenced by the engine design and the type of propellant used.
Rocket Propulsion
Rocket propulsion is a fascinating area of physics that enables rockets to travel through the atmosphere and beyond. It involves converting chemical energy from the rocket fuel into kinetic energy of the expelled gases, creating thrust.
The entire process can be broken down as follows:
  • Fuel is burnt in the rocket’s engine, creating hot gases.
  • The gases expand and are expelled through the rocket’s nozzle at high speeds.
  • The expulsion of gases generates an upward force, or thrust, that propels the rocket forward.
This mechanism is why rockets do not require air to generate thrust. They carry both fuel and an oxidizer needed for combustion. Therefore, the rocket engine works efficiently even in the vacuum of space.
Thrust in Outer Space
One of the wonders of rocket science is how rockets can operate in the vacuum environment of outer space. Unlike jet engines, rockets do not rely on atmospheric oxygen. They can produce thrust by expelling the gases generated from burning fuel.
In outer space, thrust generation relies solely on the mass flow rate and the exhaust velocity. No external air or atmospheric pressure is necessary.
  • The thrust continues to propel the rocket forward based on the internal expulsion of gases.
  • Maneuvering and steering are achieved by altering the direction of the expelled gases.
Even in the absence of air resistance or upthrust, rockets can steer through space by adjusting their nozzles or engines. Slowing down, or braking, involves reversing the direction of thrust, often by turning the rocket and firing its engines in the opposite direction, a procedure known as retro-burning.

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Most popular questions from this chapter

Two vehicles are approaching an intersection. One is a 2500-kg pickup traveling at 14.0 m/s from east to west (the \(-x\)-direction), and the other is a 1500-kg sedan going from south to north (the \(+y\) direction) at 23.0 m/s. (a) Find the \(x\)- and \(y\)-components of the net momentum of this system. (b) What are the magnitude and direction of the net momentum?

A 15.0-kg block is attached to a very light horizontal spring of force constant 500.0 N>m and is resting on a frictionless horizontal table (\(\textbf{Fig. E8.44}\)). Suddenly it is struck by a 3.00-kg stone traveling horizontally at 8.00 m/s to the right, whereupon the stone rebounds at 2.00 m/s horizontally to the left. Find the maximum distance that the block will compress the spring after the collision.

Blocks \(A\) (mass 2.00 kg) and \(B\) (mass 10.00 kg, to the right of \(A\)) move on a frictionless, horizontal surface. Initially, block \(B\) is moving to the left at 0.500 m/s and block \(A\) is moving to the right at 2.00 m/s. The blocks are equipped with ideal spring bumpers, as in Example 8.10 (Section 8.4). The collision is headon, so all motion before and after it is along a straight line. Find (a) the maximum energy stored in the spring bumpers and the velocity of each block at that time; (b) the velocity of each block after they have moved apart.

A 70-kg astronaut floating in space in a 110-kg MMU (manned maneuvering unit) experiences an acceleration of 0.029 m/s\(^2\) when he fires one of the MMU's thrusters. (a) If the speed of the escaping N\(_2\) gas relative to the astronaut is 490 m/s, how much gas is used by the thruster in 5.0 s? (b) What is the thrust of the thruster?

A 0.160-kg hockey puck is moving on an icy, frictionless, horizontal surface. At \(t\) = 0, the puck is moving to the right at 3.00 m/s. (a) Calculate the velocity of the puck (magnitude and direction) after a force of 25.0 N directed to the right has been applied for 0.050 s. (b) If, instead, a force of 12.0 N directed to the left is applied from \(t\) = 0 to \(t\) = 0.050 s, what is the final velocity of the puck?

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