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Today, we'll start by discussing pressure measurement. Who can tell me what a barometer is used for?
It measures atmospheric pressure.
Correct! A barometer helps us determine the local atmospheric pressure. If we say R is 750 mm of Hg, how do we express the atmospheric pressure in terms of Pascal?
We’d convert it using density and height.
Exactly! The formula is P = S * R. Therefore, if R = 750 mm, what is the atmospheric pressure?
It comes out to be about 100,000 Pascal.
Excellent! Remember, atmospheric pressure can change depending on altitude, and barometers are very useful for this.
Now let’s shift to understanding the isothermal process. What do we mean by isothermal?
It means the temperature remains constant.
That's right! In this process, the ideal gas equation plays a crucial role. Can anyone recall that equation?
PV = nRT!
Spot on! As we integrate from P1 to P2 and z1 to z2, we get an interesting relationship for pressure change. Can someone suggest what that results in?
It looks like it gives an exponential function.
Exactly! Pressure variation is presented as P2 = P1e^[-(Mg/RT)(Z2-Z1)]. This is important in understanding how gases respond to height differences.
Let’s explore manometers. Can someone explain how a standard manometer works?
It measures pressure relative to atmospheric pressure.
Correct! And what about differential manometers? How do they differ?
They measure pressure differences between two points.
Exactly! For example, in a water distribution system, if we check the pressure at a certain point, like 500 kPa, how would we calculate the height of water in the manometer?
We'd use the pressure divided by the density of water.
Right! The height h can be found using h = p/ρg. This means that denser liquids can help us get a much smaller height measurement.
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The section examines how pressure changes in compressible fluids, illustrating concepts using ideal gas principles under isothermal conditions. It describes the application of barometers and manometers as pressure measurement tools, emphasizing the significance of atmospheric pressure in calculations.
The discussion on pressure variations in compressible fluids primarily revolves around two processes involving perfect gases: isothermal processes and those with constant temperature gradients. An example is provided for calculating atmospheric pressure via a barometer, while the concept of pressure measurement using different devices—such as standard manometers and differential manometers—is also introduced.
PV = nRT
) becomes pivotal in deriving pressure variations. The relationship provides insights into how pressure changes when the altitude shifts in a fluid column.
Overall, this section serves to provide foundational knowledge about pressure variations in compressible fluids, essential for advanced studies in fluid mechanics.
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Now, we must also be a little aware about the pressure variations in a compressible fluid. There are 2 processes, one is perfect gas at constant temperature isothermal that we have been seeing till now. Secondly perfect gas with constant temperature gradient.
In this chunk, we start by introducing the concept of pressure variations in compressible fluids. The two processes mentioned are key to understanding how gases behave under different conditions. The first process is isothermal, where the temperature remains constant, and the second involves a temperature gradient, which means that temperature can vary along different points in the gas. Understanding these processes is essential as they form the basis for further analysis of pressure variations in gases.
Think of a balloon filled with air. When you squeeze the balloon, the air inside is compressed, and you can feel the pressure increase. If you keep the temperature of the air the same while compressing it (isothermal), the pressure inside the balloon increases according to the principles of isothermal gas behavior. Once you release the pressure and allow the balloon to return to its original shape, you're witnessing the gas returning to a state of lower pressure.
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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 where the is a function of P. So, because in gas it is PV = nRT that is the thumb rule for isothermal.
In this chunk, we delve into the isothermal process specifically. The equation PV = nRT is fundamental for understanding the behavior of gases when temperature is held constant. Here, P represents pressure, V is volume, n is the amount of substance, R is the universal gas constant, and T is the absolute temperature. The relationship showcases how pressure and volume are inversely related in a gas; as one increases, the other must decrease to keep the product constant when temperature is constant.
Imagine a sealed syringe filled with air. When you push the plunger, you decrease the volume of the air inside but at the same time, since the temperature remains constant, the pressure inside the syringe increases. This principle is applied frequently in various technologies, such as in internal combustion engines where air is compressed before ignition.
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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 P1 to P2, and z1 to z2 simple integration, and if you integrate this, we are going to get because it is dp / p.
This chunk introduces the mathematical approach needed to evaluate pressure variation in an isothermal process. By integrating the change in pressure (dp) and the change in elevation (dz) over the defined limits (from point 1 to point 2), we can obtain a relationship between the initial and final pressures. The integration leads to the logarithmic relationship, which is a common mathematical result in fluid mechanics showing how pressure changes in a fluid column.
Consider water flowing down a slide. If you were to measure the water pressure at the top versus the bottom of the slide, this pressure difference can be represented mathematically similar to how we integrate to find the change in pressure in our equation. As the water descends, the pressure decreases due to the gravitational effects, similar to how we derive relationships in our equations.
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So, the pressure at point 2 in a constant temperature will be given as p = p1 e^[-(Mg/RaTs)(Z2-Z1)].
Here, we present the final equation derived for pressure at point 2 during an isothermal process. The equation illustrates how the initial pressure (p1) exponentially decreases based on the height difference (Z2 - Z1) and the constants for the gas used. This relationship is crucial in various applications, showing how pressure is affected by changes in elevation within a fluid or gas amidst constant temperature conditions.
If you think of climbing a mountain, as you ascend (which corresponds to an increase in height Z2 compared to Z1), the air pressure decreases. This drop in pressure as you gain altitude can be explained such that it follows the mathematical relationship derived, where your starting pressure is higher (like at sea level) and drops exponentially as you climb.
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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.
This chunk provides an overview of various devices used for measuring pressure. Barometers measure atmospheric pressure, manometers measure the pressure of liquids and gases relative to a reference pressure, particularly atmospheric pressure, and differential manometers measure the pressure difference between two points. Understanding these devices is key for applying the principles of fluid mechanics in real-world scenarios.
Imagine measuring the tire pressure of a car. A pressure gauge provides direct readings of the tire's internal pressure. This pressure can be compared to the atmospheric pressure around it, similar to how manometers compare pressures in fluid systems. Knowing these pressures helps ensure safe driving conditions.
Learn essential terms and foundational ideas that form the basis of the topic.
Key Concepts
Atmospheric pressure: The pressure exerted by the weight of the air above.
Isothermal conditions: The state in which temperature remains constant during a process.
Pressure measurement: Techniques used to quantify fluid pressures relative to atmospheric conditions.
Gauge pressure: The measure of pressure relative to the ambient atmospheric pressure.
See how the concepts apply in real-world scenarios to understand their practical implications.
Using a barometer where mercury R is stated as 750 mm to find atmospheric pressure as approximately 100,000 Pascal.
A water distribution system where pressure is at 500 kPa, calculated by determining the water manometer height at around 51 m.
Use mnemonics, acronyms, or visual cues to help remember key information more easily.
Measure the air up high, a barometer will tell you why!
Imagine a scientist holding a barometer in a desert, watching how the mercury level changes as they climb to higher ground, understanding the relationship between altitude and pressure.
Remember P = S * R for calculating pressure.
Review key concepts with flashcards.
Review the Definitions for terms.
Term: Barometer
Definition:
A device used to measure atmospheric pressure.
Term: Isothermal Process
Definition:
A thermodynamic process that occurs at a constant temperature.
Term: Manometer
Definition:
A device used to measure the pressure of a fluid relative to atmospheric pressure.
Term: Gauge Pressure
Definition:
The pressure measured relative to atmospheric pressure.
Term: Piezometric Head
Definition:
The height of a fluid column that represents the pressure at a certain point in a fluid.