Assuming that atmospheric temperature decreases with increasing altitude at a uniform rate of \(0.0065 \mathrm{~K} \cdot \mathrm{m}^{-1}\), determine the atmospheric pressure at an altitude of \(7.5 \mathrm{~km}\) if the temperature and pressure at sea level are \(15^{\circ} \mathrm{C}\) and \(101.5 \mathrm{kPa}\) respectively. \(\left(R=287 \mathrm{~J} \cdot \mathrm{kg}^{-1} \cdot \mathrm{K}^{-1}\right)\)

Short Answer

Expert verified
The atmospheric pressure at an altitude of 7.5 km is approximately 50.54 kPa.

Step by step solution

01

- Convert Sea Level Temperature

Convert the given sea level temperature from Celsius to Kelvin. The formula for this conversion is \(T(\text{K}) = T(^{\text{∘}C}) + 273.15\)Given:\[T_0 = 15^{\text{∘}C} = 15 + 273.15 = 288.15 \text{K}\]
02

- Calculate Temperature at Altitude

Use the temperature lapse rate to calculate the temperature at the given altitude. The formula is \( T = T_0 - L h \) where \(L\) is the lapse rate (\(0.0065 \text{ K }\text{m}^{-1}\)), \(h\) is the altitude\[ T = 288.15 \text{K} - (0.0065 \text{K}/\text{m}) \times 7500 \text{m} \]\[ T = 288.15 \text{K} - 48.75 \text{K} \]\[ T = 239.4 \text{K} \]
03

- Use the Barometric Formula

Plug the values into the barometric formula to find the pressure at altitude. The formula is \[ P = P_0 \times \bigg(1 - \frac{Lh}{T_0} \bigg)^{\frac{gM}{RL}} \]Given:\(P_0 = 101.5 \text{kPa}\), \(L = 0.0065 \text{ K }\text{m}^{-1}\), \(h = 7500 \text{m}\), \(T_0 = 288.15 \text{K}\), \(R = 287 \text{ J }\text{kg}^{-1}\text{K}^{-1} \), and gravitational constant \( g = 9.81 \text{m}/\text{s}^2 \), and molar mass of dry air \( M = 0.029 \text{kg}\text{mol}^{-1} \).\[ P = 101.5 \text{kPa} \times \bigg( 1 - \frac{0.0065 \times 7500}{288.15} \bigg)^{\frac{9.81 \times 0.029}{287 \times 0.0065}} \]\[ P = 101.5 \text{kPa} \times \bigg(1 - 0.169119 \bigg)^{5.255877} \]\[ P = 101.5 \text{kPa} \times (0.830881)^{5.255877} \]\[ P \approx 101.5 \text{kPa} \times 0.498 \]\[ P \approx 50.54 \text{kPa} \]

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Key Concepts

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

atmospheric pressure
Atmospheric pressure is the force exerted by the weight of air in the atmosphere. It decreases with altitude because there is less air above the point of measurement. At sea level, this pressure is about 101.5 kPa. Atmospheric pressure impacts weather patterns, altitude sickness, and even the functioning of the human body. Everyday applications include weather forecasting and aircraft operations.
temperature lapse rate
The temperature lapse rate is the rate at which atmospheric temperature decreases with an increase in altitude. It is typically taken as a constant for simplicity, often around 0.0065 K/m. This means for every meter you go up, the temperature drops by 0.0065 K. This rate helps in weather prediction, climate modeling, and determining atmospheric conditions at different altitudes.
barometric formula
The barometric formula is a mathematical equation used to calculate the pressure at a given altitude. It takes into account the sea level pressure, altitude, temperature lapse rate, gravitational acceleration, gas constant, and molar mass of air.The formula is:\[ P = P_0 \times \bigg(1 - \frac{Lh}{T_0}\bigg)^{\frac{gM}{RL}} \]Where:
  • P is the pressure at altitude
  • P₀ is the sea level pressure
  • L is the lapse rate
  • h is the altitude
  • T₀ is the sea level temperature in Kelvin
  • g is the acceleration due to gravity
  • R is the gas constant for dry air
  • M is the molar mass of Earth's air
This formula is vital for aviation, meteorology, and environmental science.
altitude effects on pressure
As altitude increases, atmospheric pressure decreases. This happens because there are fewer air molecules at higher altitudes, reducing the weight of air above. At lower altitudes, air is denser, resulting in higher pressure. This effect is crucial for understanding weather patterns, planning air travel, and assessing altitude-related health risks. It also influences how oxygen is available in high-altitude regions and affects how engines operate in different conditions.

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Most popular questions from this chapter

A test vehicle contains a U-tube manometer for measuring differences of air pressure. The manometer is so mounted that, when the vehicle is on level ground, the plane of the U is vertical and in the fore-and-aft direction. The arms of the \(\mathrm{U}\) are \(60 \mathrm{~mm}\) apart, and contain alcohol of relative density \(0.79 .\) When the vehicle is accelerated forwards down an incline at \(20^{\circ}\) to the horizontal at \(2 \mathrm{~m} \cdot \mathrm{s}^{-2}\) the difference in alcohol levels (measured parallel to the arms of the \(\mathrm{U}\) ) is \(73 \mathrm{~mm}\), that nearer the front of the vehicle being the higher. What is the difference of air pressure to which this reading corresponds?

A hollow cylinder with closed ends is \(300 \mathrm{~mm}\) diameter and \(450 \mathrm{~mm}\) high, has a mass of \(27 \mathrm{~kg}\) and has a small hole in the base. It is lowered into water so that its axis remains vertical. Calculate the depth to which it will sink, the height to which the water will rise inside it and the air pressure inside it. Disregard the effect of the thickness of the walls but assume that it is uniform and that the compression of the air is isothermal. (Atmospheric pressure \(=101.3 \mathrm{kPa}\) )

An open-topped tank, in the form of a cube of \(900 \mathrm{~mm}\) side, has a mass of \(340 \mathrm{~kg}\). It contains \(0.405 \mathrm{~m}^{3}\) of oil of relative density \(0.85\) and is accelerated uniformly up a long slope at arctan (1/3) to the horizontal. The base of the tank remains parallel to the slope, and the side faces are parallel to the direction of motion. Neglecting the thickness of the walls of the tank, estimate the net force (parallel of the slope) accelerating the tank if the oil is just on the point of spilling.

A circular opening \(1.2 \mathrm{~m}\) in diameter in the vertical side of a reservoir is closed by a disc which just fits the opening and is pivoted on a shaft along its horizontal diameter. Show that, if the water level in the reservoir is above the top of the disc, the turning moment on the shaft required to hold the disc vertical is independent of the head of water. Calculate the amount of this moment.

An open channel has a cross-section in the form of an equilateral triangle with \(2.5 \mathrm{~m}\) sides and a vertical axis of symmetry. Its end is closed by a triangular vertical gate, also with \(2.5 \mathrm{~m}\) sides, supported at each corner. Calculate the horizontal thrust on each support when the channel is brim-full of water.

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