Problem 57
Question
\(\bullet\) A \(70-\mathrm{kg}\) astronaut floating in space in a \(110-\mathrm{kg}\) MMU (manned maneuvering unit) experiences an acceleration of 0.029 \(\mathrm{m} / \mathrm{s}^{2}\) when he fires one of the MMU's thrusters. (a) If the speed of the escaping \(\mathrm{N}_{2}\) gas relative to the astronaut is 490 \(\mathrm{m} / \mathrm{s}\) , how much gas is used by the thruster in 5.0 \(\mathrm{s} \%\) (b) What is the thrust of the thruster?
Step-by-Step Solution
Verified Answer
(a) Approx. 0.053 kg of gas, (b) Thrust is 5.22 N.
1Step 1: Determine the Total Mass of the System
To find the total mass, sum up the mass of the astronaut and the mass of the MMU:\[m_{total} = m_{astronaut} + m_{MMU} = 70 \, \text{kg} + 110 \, \text{kg} = 180 \, \text{kg}\]
2Step 2: Calculate the Thrust of the Thruster
Use Newton's second law to find the force (thrust) applied by the thruster.\[F = m_{total} \times a = 180 \, \text{kg} \times 0.029 \, \text{m/s}^2 = 5.22 \, \text{N}\]This force is the thrust provided by the MMU thruster.
3Step 3: Determine the Mass of Gas Used
The momentum change equals the thrust times the time, and is also equal to the change in momentum of the gas. Use the momentum conservation principle:\[F \times t = m_{gas} \times v_{gas}\]Solving for \(m_{gas}\):\[m_{gas} = \frac{F \times t}{v_{gas}}\]With the given values:\[m_{gas} = \frac{5.22 \, \text{N} \times 5.0 \, \text{s}}{490 \, \text{m/s}} \approx 0.053 \, \text{kg}\]This is the mass of the gas used by the thruster in 5 seconds.
Key Concepts
Momentum ConservationThrust CalculationSpace Mechanics
Momentum Conservation
A fundamental principle in physics, momentum conservation is pivotal in understanding how objects move. It states that the total momentum of a closed system remains constant if no external forces act on it. In the context of space mechanics, where external forces are minimal, this becomes essential. When the astronaut and the manned maneuvering unit (MMU) fire their thruster, the escaping gases provide thrust by exerting a force in one direction, propelling the astronaut in the opposite direction due to conservation of momentum. Using the equation for momentum conservation, we find that the momentum transferred to the gas equals the momentum gained by the astronaut and MMU:
- Initial Momentum = Final Momentum
- \[ m_{gas} \times v_{gas} = (m_{total}) \times \Delta v \]
Thrust Calculation
The calculation of thrust is critical in applications such as rocketry and space travel. Thrust is the force produced by the thruster, allowing movement or acceleration of the system. Using Newton's Second Law, we determine the thrust by multiplying the total mass of the astronaut and MMU by the acceleration experienced:
- \[ F = m_{total} \times a \]
- In our case, \( F = 180 \times 0.029 = 5.22 \text{ N} \).
Space Mechanics
Space mechanics deals with the motion of objects in the vacuum of space, where traditional forces such as gravity and friction are negligible. Understanding how to control and predict the path of objects is essential. When dealing with space mechanics, concepts like momentum conservation and thrust are crucial. The forces at play are extremely precise and must be carefully calculated and executed for successful missions.
Without the influence of atmospheric forces, MMUs gain importance. They offer stability and control by using thrusters to adjust their position and orientation. This machine exemplifies space mechanics, relying on principles like controlled thrust and efficient propulsion systems to move in desired directions. The astronaut's ability to control their trajectory precisely showcases space mechanics' practical application. Implementing Newton's laws in a microgravity environment shows how theoretical physics translates into real-world action, a necessity for advancing space exploration and travel.
Without the influence of atmospheric forces, MMUs gain importance. They offer stability and control by using thrusters to adjust their position and orientation. This machine exemplifies space mechanics, relying on principles like controlled thrust and efficient propulsion systems to move in desired directions. The astronaut's ability to control their trajectory precisely showcases space mechanics' practical application. Implementing Newton's laws in a microgravity environment shows how theoretical physics translates into real-world action, a necessity for advancing space exploration and travel.
Other exercises in this chapter
Problem 55
A rocket is fired in deep space, where gravity is negligible. If the rocket has an initial mass of 6000 \(\mathrm{kg}\) and ejects gas at a relative velocity of
View solution Problem 56
\(\bullet\) In outer space, where gravity is negligible, a \(75,000 \mathrm{kg}\) rocket (including \(50,000 \mathrm{kg}\) of fuel) expels this fuel at a steady
View solution Problem 58
\(\bullet\) In 1.00 second an automatic paintball gun can fire 15 balls, each with a mass of \(0.113 \mathrm{g},\) at a muzzle velocity of 88.5 \(\mathrm{m} / \
View solution Problem 59
\(\bullet\) In a volcanic eruption, a 2400 -kg boulder is thrown vertically upward into the air. At its highest point, it suddenly explodes (due to trapped gase
View solution