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A meteorite hits the upper atmosphere at 10000 \(\mathrm{ft} / \mathrm{s}\) where the pressure is \(0.1 \mathrm{~atm}\) and temperature \(-40 \mathrm{~F}\). How hot does the air become right in front of the meteorite assuming no heat transfer in this adiabatic stagnation process?

Short Answer

Expert verified
The air temperature becomes approximately 4855 K.

Step by step solution

01

Understand the problem

We are asked to determine the temperature right in front of the meteorite. This requires understanding the adiabatic process in the context of high-speed aerodynamic heating, where kinetic energy is converted into thermal energy.
02

Convert units

Convert the initial conditions to SI units. The velocity is given as 10000 ft/s, which is approximately 3048 m/s (since 1 ft = 0.3048 m). The temperature \[-40 ^\circ \text{F} = \frac{5}{9}(-40 - 32) ^\circ \text{C} = -40 ^\circ \text{C}\]. Then, convert to Kelvin: \[-40 ^\circ \text{C} + 273.15 = 233.15\ K\].
03

Apply the adiabatic stagnation temperature formula

Use the adiabatic stagnation temperature formula: \[ T_0 = T + \frac{v^2}{2c_p} \]. Here, \(T\) is the initial temperature, \(v\) is the velocity, and \(c_p\) is the specific heat capacity at constant pressure for air (approximately 1005 J/kg·K).
04

Calculate

Plug in the values: \[ T_0 = 233.15 \ K + \frac{(3048)^2}{2 \times 1005} \approx 233.15 \ K + 4621.74 \ K \approx 4854.89 \ K\].
05

Interpret the results

The air temperature right in front of the meteorite significantly increases due to the high entry speed, resulting in a temperature of approximately 4855 K. This temperature indicates the intense thermal energy generated by the conversion of kinetic energy into heat.

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Key Concepts

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

Adiabatic Stagnation Temperature
When dealing with fast-moving objects like meteorites entering the Earth's atmosphere, it's crucial to understand adiabatic stagnation temperature. This concept explains how air heats up rapidly before a moving object due to compression and the absence of heat exchange with the surroundings. The adiabatic process assumes no heat transfer, making the object's velocity a key factor in heating.

In this context, adiabatic stagnation temperature can be calculated using the formula: \[ T_0 = T + \frac{v^2}{2c_p} \]where:
  • \( T_0 \) - Adiabatic stagnation temperature (final temperature)
  • \( T \) - Initial temperature
  • \( v \) - Velocity of the object (meteorite in this case)
  • \( c_p \) - Specific heat capacity of the surrounding medium (air)
Understanding this formula is fundamental in predicting temperature changes during high-speed atmospheric entries, revealing how kinetic energy is substantially converted into thermal energy.
Kinetic Energy Conversion
The phenomenon of kinetic energy conversion explains the dramatic rise in temperature experienced by objects entering the Earth's atmosphere at tremendous speeds. When a meteorite hits the atmosphere, its velocity converts some of its kinetic energy into thermal energy, increasing the surrounding air temperature.

Let's think about kinetic energy: it is given by the expression \( \frac{1}{2}mv^2 \), where \( m \) is mass and \( v \) is velocity. For an adiabatic process like a meteorite entry, this immense energy transformation surfaces as surrounding air temperatures, creating heat comparable to conditions seen in space missions or rocket launches. Understanding this conversion is fundamental in predicting risks and planning space-related activities.
Specific Heat Capacity
Specific heat capacity is a crucial concept in physics, especially when calculating thermal changes in an adiabatic process. It determines how much heat an object or substance can store and plays an essential role in calculations involving temperature changes. In atmospheric sciences, the specific heat capacity of air, usually denoted as \( c_p \), significantly influences how violently air can heat up.

In most cases, for dry air at constant pressure, it's approximately \( 1005 \text{ J/kg·K} \). This numerical value helps in calculating the final temperature of objects like meteorites or spacecraft during atmospheric entry, ensuring accurate predictions of temperature changes due to kinetic energy conversion.
Atmospheric Entry Conditions
Atmospheric entry conditions encompass various factors impacting the experience of objects entering the Earth’s atmosphere. This includes velocity, atmospheric pressure, temperature, and composition. When a meteorite enters the thin upper layers of the atmosphere, it encounters drastically different conditions than those at sea level.

Entry speed and altitude significantly influence the thermal dynamics. At high speeds, like 10000 ft/s (or roughly 3048 m/s), these conditions translate into extreme heating as velocity converts kinetic energy into heat. Additionally, factors like pressure, which is notably lower at high altitudes (0.1 atm in this case), and temperature (-40 °F), further dictate the aerodynamic heating.

Understanding these conditions is key in predicting how pieces of space debris will interact with our atmosphere, aiding in the design of thermal shields and ensuring re-entry safety for spacecraft.

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Most popular questions from this chapter

A pipe flows water at \(15^{\circ} \mathrm{C}\) from one building to another. In the winter the pipe loses an estimated \(500 \mathrm{~W}\) of heat transfer. What is the minimum required mass flow rate that will ensure that the water does not freeze (i.e., reach \(0^{\circ} \mathrm{C}\) )?

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