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Today, we're going to discuss atmospheric pressure and how we measure it. Can anyone tell me what a barometer does?
A barometer measures atmospheric pressure?
Exactly! A barometer can measure how much pressure the air is exerting on us. Let's think about the relationship: when air pressure increases, what happens to the reading on the barometer?
It goes up!
Correct! And what unit do we typically use for this measurement?
Millimeters of mercury?
Right again! This is also known as Hg. Now, when R is 750 mm of Hg, how would you determine local atmospheric pressure?
By using the piezometric head equation, I think?
Yes, and remember that we can express pressure at point 1 using P = S * R. Great job, everyone! Let's proceed to the next concept.
Now, let’s dive into isothermal processes in perfect gases. Who can remind us what isothermal means?
It means the temperature stays constant!
Exactly! And for an ideal gas, we can use the equation PV = nRT. What does each symbol represent?
P is pressure, V is volume, n is the number of moles, R is the gas constant, and T is temperature.
Correct! Now, when we differentiate this, we get dp/dp = 1/P. How does integrating this from P1 to P2 help us?
It helps us calculate the pressure at point 2 using the natural logarithm!
Fantastic! The formula becomes P = P1 * exp[-(Mg / RaT * (Z2 - Z1))]. Can anyone explain what M represents?
M is the molecular mass, right?
Exactly! You’re all doing great. In summary, understanding isothermal processes is crucial for applications in various engineering fields.
Let’s take a look at the devices we use to measure pressure. Can anyone name some of them?
Barometers and manometers?
Good! A barometer measures atmospheric pressure while a manometer can measure pressure differentials. How do these devices relate to our earlier discussions about pressure in fluids?
They help us understand how pressure varies with fluid height and density!
Exactly! By using denser liquids like mercury in manometers, we can measure higher pressures with less height. Why do you think mercury is preferred?
Because it has a higher density, so it rises less for the same pressure?
Exactly correct! Let’s reinforce that knowledge with a few examples about how to use manometers practically.
Alright, let’s tackle some pressure calculation examples. If we have a pressure of 500 kPa, how far will water rise in a manometer full of water?
We could use the formula h = P / (density * g)! That should give us the height.
Exactly! Now, substituting in our values, what do we find?
It will give us about 51 m.
Well done! What would that height be if we used mercury instead?
It will be much less since mercury is denser!
Correct! That means we’ll have to account that in our calculations. Balancing pressure in fluids is vital to applications in engineering.
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The section explains isothermal processes within the context of perfect gases, detailing the piezometric equations and methods of measuring atmospheric pressure using barometers and manometers. It emphasizes the relationship between pressure, temperature, and volume and introduces formulas for calculating pressure in these scenarios.
In this section, the concepts of isothermal processes—where the temperature remains constant—and perfect gases are explored in detail. We begin by familiarizing ourselves with pressure measurement devices like barometers and manometers, explaining how these are instrumental in understanding local atmospheric pressure. We employ the hyostatic principle to arrive at the isothermal equation, P = P1 * exp[-(Mg / R * T * (Z2 - Z1))], which describes pressure changes when temperature is kept constant in perfect gases. The importance of gauging pressure in fluid mechanics is emphasized, with examples being provided to challenge students to apply these principles in practical situations.
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Now, we are going to do perfect gas at constant temperature that is isothermal process, we start with the same old equation. And where gamma is a function of P. So, because in gas it is PV = nRT that is the thumb rule for isothermal. So, it can be written as n*M /V or in other terms we can write it as pM / RT, M is the molecular mass which we have seen in lecture number 1.
An isothermal process is a thermodynamic process in which the temperature of the system remains constant. For perfect gases, this can be expressed using the equation PV = nRT, where P is pressure, V is volume, n is the amount of gas in moles, R is the universal gas constant, and T is the absolute temperature. Here, M represents the molecular mass of the gas. This means that if you know the number of moles and the temperature, you can calculate the product of pressure and volume.
Think of a balloon filled with air. If you squeeze the balloon (decreasing the volume), the air inside gets compressed, increasing the pressure. However, if you then let the balloon return to its original shape without adding heat, the temperature of the air doesn’t change significantly, making the process isothermal.
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So, dp will be , so this is. Correct? Because we already seen here, we just multiplied the density with G here. So, now, we start simply integrating from P 1 to P 2, and z1 to z2 simple integration, and if you integrate this, we are going to get because it is dp / p. So, that becomes ln (p2/p1) and dz is a simple integration yielding (Z 2 - Z 1).
In isothermal processes, the relationship between pressure and height can be derived through integration. By considering the equation for pressure as a function of height, you can see that as you integrate from an initial pressure P1 to a final pressure P2, the equation simplifies to involve logarithms. This gives a clear way to calculate how the pressure changes with height in an isothermal environment.
Imagine a sealed container of air. If you were to lift this container up a mountain, the pressure inside would change with the height due to the decrease in external atmospheric pressure. Using the integration we discussed, you could mathematically predict how much pressure drops as you ascend.
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So, the pressure at point 2 in a constant temperature will be given as 𝑝 = 𝑝 e−[𝑀𝑔 𝑅𝑎 𝑇𝑠𝑔 (𝑍2−𝑍1)].
This equation shows how the pressure p at height Z2 is related to the pressure p1 at height Z1. The exponential part represents how gravity and the temperature of the gas influence the pressure. Essentially, it indicates that as you go higher (i.e., Z2 increases), the pressure decreases exponentially due to gravitational effects on the gas molecules.
Think of a hot air balloon. As the balloon rises, the pressure of the air inside decreases. The temperature needs to be maintained to keep the balloon floating. If the air inside cools too much, it will start to drop because the pressures equalize.
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Pressure measurement devices, we have discussed one already barometers, there are manometers, a standard manometer or a differential manometer and the pressure transducers.
There are several instruments to measure pressure. A barometer is used to measure atmospheric pressure, while manometers can measure pressure relative to atmosphere or the pressure difference between two points. These devices employ different liquids to gauge pressure, such as water or mercury, each selected based on density and measurement accuracy.
Consider a barometer as a weather forecasting tool. When you check the barometer and see it drop, it's likely that rain is on the way because low atmospheric pressure typically signals weather changes.
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For standard manometers, what is the pressure? So how it works is very simple example. So, what is if we are asked, what is the pressure at A given the height, more importantly we should mention what is the gauge pressure.
When measuring pressure in contexts like water distribution systems, gauge pressure is commonly used, which excludes atmospheric pressure. Calculating pressure involves knowing either the height of the liquid column in the manometer or using fluid density. This way, you can determine how high a column of liquid like water can rise based on the pressure applied.
Imagine a simple water fountain. The pressure driving the water up through the fountain changes based on the depth of the water source and any restrictions in the piping. Understanding these pressures allows you to design a fountain that works correctly without overflows or underwhelming spray heights.
Learn essential terms and foundational ideas that form the basis of the topic.
Key Concepts
Isothermal Processes: These processes occur at constant temperature, and the relationship between pressure and volume can be expressed mathematically.
Perfect Gas: An idealized gas that precisely follows gas laws, allowing for simpler calculations.
Pressure Measurement: Various devices like barometers and manometers are utilized to measure atmospheric and gauge pressures.
Pressure Calculations: Understanding pressure variations is essential for engineers, and calculations can involve height, density, and pressure relationships.
See how the concepts apply in real-world scenarios to understand their practical implications.
Calculating the height of water in a manometer connected to a pipe with a pressure of 500 kPa involves using the density of water and gravity to determine how high the water will rise.
Using the formula P = P1 * exp[-(Mg / RaT * (Z2 - Z1))], the pressure at a specific point in an isothermal process can be computed, highlighting the relationship between height and pressure change.
Use mnemonics, acronyms, or visual cues to help remember key information more easily.
For pressure in the air, a barometer we share, with mercury so dense, it measures immense.
Imagine a scientist standing in a lab with a shiny barometer. Every time the weather changes, the mercury rises or falls, guiding the scientist to predict rain with precision and awe.
To remember the components: P - Pressure, V - Volume, n - Moles, R - Gas constant, T - Temperature, think 'Puppy Visits New Raccoons Terribly.'
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Review the Definitions for terms.
Term: Isothermal Process
Definition:
A process that occurs at constant temperature.
Term: Perfect Gas
Definition:
An idealized gas that perfectly follows the gas laws.
Term: Atmospheric Pressure
Definition:
The pressure exerted by the weight of the atmosphere.
Term: Piezometric Head
Definition:
The height of a fluid column that represents the pressure at a point.
Term: Barometer
Definition:
A device used to measure atmospheric pressure.
Term: Manometer
Definition:
A device used to measure the pressure of a liquid.
Term: Pressure Transducer
Definition:
A device that converts pressure into an electrical signal.
Term: Molecular Mass (M)
Definition:
The mass of a single molecule of a substance.
Term: Density
Definition:
Mass per unit volume of a substance.
Term: Gauge Pressure
Definition:
Pressure relative to atmospheric pressure.