A spherical, helium-filled balloon of diameter \(800 \mathrm{~mm}\) is to be used to carry meteorological instruments to a height of \(6000 \mathrm{~m}\) above sea level. The instruments have a mass of \(60 \mathrm{~g}\) and negligible volume, and the balloon itself has a mass of \(100 \mathrm{~g}\). Assuming that the balloon does not expand and that atmospheric temperature decreases with increasing altitude at a uniform rate of \(0.0065 \mathrm{~K} \cdot \mathrm{m}^{-1}\), determine the mass of helium required. Atmospheric pressure and temperature at sea level are \(15^{\circ} \mathrm{C}\) and \(101 \mathrm{kPa}\) respectively; for air, \(R=287 \mathrm{~J} \cdot \mathrm{kg}^{-1} \cdot \mathrm{K}^{-1}\)

Short Answer

Expert verified
0.024 kg of helium is required.

Step by step solution

01

Determine the volume of the balloon

The diameter of the balloon is given as 800 mm, which is 0.8 meters. The volume of a sphere is calculated using the formula:\[ V = \frac{4}{3} \pi r^3 \] where \[ r = \frac{d}{2} = \frac{0.8}{2} = 0.4 \text{ m} \]Now, substitute the value of r:\[ V = \frac{4}{3} \pi (0.4)^3 \approx 0.268 \text{ m}^3 \]
02

Calculate the pressure and temperature at 6000 meters altitude

The temperature decreases with altitude at a rate of 0.0065 K/m. The initial temperature at sea level is 15°C, or 288.15 K. The altitude given is 6000 meters. Therefore, the temperature at 6000 meters is:\[ T = 288.15 - (0.0065 \times 6000) = 249.15 \text{ K} \] To find the pressure at 6000 meters, use the barometric formula:\[ P = P_0 \left(1 - \frac{Lh}{T_0} \right)^{\frac{gM}{RL}} \] where \( P_0 = 101 \text{ kPa} \), \(L = 0.0065 \text{ K/m} \), \(h = 6000 \text{ m} \), \(T_0 = 288.15 \text{ K} \), \(g = 9.8 \text{ m/s}^2\), \(M = 0.029 \text{ kg/mol} \), and \(R = 8.314 \text{ J/(mol*K)} \). Substituting in these values:\[ P = 101000 \left(1 - \frac{(0.0065)(6000)}{288.15} \right)^{\frac{(9.8)(0.029)}{(8.314)(0.0065)}} \approx 47.349 \text{ kPa} \]
03

Apply the ideal gas law to find the mass of helium required

The ideal gas law is given by:\[ PV = mRT \] Rearrange to solve for \( m \):\[ m = \frac{PV}{RT} \] Substitute the known values:\[ P = 47349 \text{ Pa} \]\[ V = 0.268 \text{ m}^3 \]\[ R = 2077 \text{ J/(kg*K)} \] (specific gas constant for helium)\[ T = 249.15 \text{ K} \]\[ m = \frac{47349 \times 0.268}{2077 \times 249.15} \approx 0.024 \text{ kg} \]
04

Find the total mass the balloon can carry and validate

The total mass the balloon can carry is the sum of the mass of the instruments and the mass of the balloon:\[ m_{total} = 0.024 + 0.06 + 0.1 = 0.184 \text{ kg} \]Since the required mass of helium is much smaller compared to the carrying capacity, it confirms there are no calculation errors.

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Key Concepts

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

Ideal Gas Law
The Ideal Gas Law is a fundamental equation for understanding the behavior of gases. The law is represented as \(PV = nRT\), where \(P\) represents pressure, \(V\) is volume, \(n\) is the number of moles of gas, \(R\) is the universal gas constant, and \(T\) is the temperature in Kelvin. In many practical exercises, we rearrange the formula to solve for different variables. For example, to find the mass of a gas, we can use the form \(m = \frac{PV}{RT}\), where \(m\) is the mass and \(R\) is replaced by the specific gas constant for the particular gas (e.g., helium has \(R = 2077 \text{ J/(kg*K)} \). Understanding this law allows us to calculate how gases behave under different pressures, volumes, and temperatures.
Atmospheric Pressure
Atmospheric pressure is the force exerted by the weight of air on the Earth's surface and objects at different altitudes. It decreases with altitude because there is less air above to exert force. At sea level, the standard atmospheric pressure is approximately 101 kPa. To calculate atmospheric pressure at a higher altitude, such as 6000 meters, we can use the barometric formula: \[ P = P_0 \bigg(1 - \frac{Lh}{T_0} \bigg)^{\frac{gM}{RL}} \] where \(P_0\) is the initial pressure, \(L\) is the temperature lapse rate, \(h\) is the altitude, \(T_0\) is the sea level temperature, \(g\) is the acceleration due to gravity, \(M\) is the molar mass of Earth's air, and \(R\) is the gas constant. Substituting these values, we find the pressure decreases significantly at higher altitudes.
Density and Volume Calculations
Understanding density and volume is crucial for problems involving buoyancy and gas behavior. The volume of a sphere, such as a balloon, is calculated using \[ V = \frac{4}{3} \pi r^3 \] where \(r\) is the radius. For our 800 mm diameter balloon, the radius \(r\) is 0.4 meters, giving a volume of approximately 0.268 cubic meters. Density is the mass per unit volume, usually expressed as \( \rho = \frac{m}{V}\). Knowing the mass and volume of the gas inside the balloon helps determine its buoyancy, directly affecting whether it can carry additional instruments and rise to the desired altitude.
Temperature Variation with Altitude
Temperature decreases with altitude at a rate known as the lapse rate, typically around 0.0065 K/m in the troposphere. To find the temperature at a given altitude, we use this relationship. Starting with the sea level temperature (15°C or 288.15 K), we can determine the temperature at 6000 meters: \[ T = 288.15 - (0.0065 \times 6000) = 249.15 \text{ K} \] This cooling effect is crucial for accurate pressure calculations and understanding how gas volume and density change with altitude, which affects balloon buoyancy and flight mechanics.

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Most popular questions from this chapter

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 solid cylinder, \(1 \mathrm{~m}\) diameter and \(800 \mathrm{~mm}\) high, is of uniform relative density \(0.85\) and floats with its axis vertical in still water. Calculate the periodic time of small angular oscillations about a horizontal axis.

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. \(\left(R=287 \mathrm{~J} \cdot \mathrm{kg}^{-1} \cdot \mathrm{K}^{-1}\right)\)

A tank with vertical sides contains water to a depth of \(1.2 \mathrm{~m}\) and a layer of oil \(800 \mathrm{~mm}\) deep which rests on top of the water. The relative density of the oil is \(0.85\) and above the oil is air at atmospheric pressure. In one side of the tank, extending through its full height, is a protrusion in the form of a segment of a vertical circular cylinder. This is of radius \(700 \mathrm{~mm}\) and is riveted across an opening \(500 \mathrm{~mm}\) wide in the plane wall of the tank. Calculate the total horizontal thrust tending to force the protrusion away from the rest of the tank and the height of the line of action of this thrust above the base of the tank.

A canal lock is \(6 \mathrm{~m}\) wide and has two vertical gates which make an angle of \(120^{\circ}\) with each other. The depths of water on the two sides of the gates are \(9 \mathrm{~m}\) and \(2.7 \mathrm{~m}\) respectively. Each gate is supported on two hinges, the lower one being \(600 \mathrm{~mm}\) above the bottom of the lock. Neglecting the weight of the gates themselves, calculate the thrust between the gates and the height of the upper hinges if the forces on them are to be half those on the lower hinges.

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