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Let's start by discussing pressure in static fluids. When a fluid is at rest, what happens to shear stress?
It becomes zero, right?
Correct! So, the only stress that acts on the control surface is normal stress, which we define as pressure. Can anyone tell me the definition of pressure in a fluid?
Pressure is force per unit area acting normal to the surface.
Exactly! And how do we represent this pressure mathematically for a point in a fluid?
We represent it as P(x, y, z).
Great! Now, remember the acronym 'PGA' - Pressure Gradients Allow us to understand variations in fluid pressure. Can anyone explain why pressure is only a function of depth in static fluids?
Because pressure increases with depth due to the weight of the fluid above!
Well done! So, remember, in static fluids, pressure varies with depth, not horizontally. This is a key point as we move forward.
Now, let’s discuss control volumes. What do we ascertain from analyzing forces in these control volumes at rest?
The total forces acting should be zero since the fluid is at rest.
Correct! The sum of body forces like gravity and surface pressures must balance. Can anyone explain how we compute these forces from pressure?
We multiply the pressure by the area over which it acts!
Right, now let's relate this to gravity forces. Can anyone tell me how gravity influences pressure in the z-direction?
Pressure increases linearly with z depth because of the weight of the fluid above.
That's an excellent insight! Remember 'GAP' - Gravity Affects Pressure. This will help solidify your understanding of how pressure behaves at various depths.
So the pressure gradient can be thought of as the change in pressure with respect to depth?
Exactly! You’re all doing great in understanding these foundational concepts!
Let's transition to discussing types of pressure. Can anyone explain the difference between gauge pressure and absolute pressure?
Gauge pressure is measured relative to atmospheric pressure, while absolute pressure measures from a perfect vacuum.
Correct! An easy way to think of it is 'Gauge is Grand, Absolute is Actual.' Why is this distinction important in engineering?
Because most applications deal with atmospheric pressure, not in a vacuum!
Exactly! So when we calculate pressures in real-world applications, we primarily deal with gauge pressures. Do you all understand how we calculate absolute pressure from gauge pressure?
We add the atmospheric pressure to gauge pressure!
Perfect! Keep in mind that understanding these terms is crucial as they will come up in various fluid dynamics problems you'll encounter.
Now, let’s look into hydrostatic pressure distribution. Can someone describe how pressure behaves in a fluid rest scenario?
Pressure varies linearly with depth in the vertical direction.
Great observation! The formula P = ρgz reflects this relationship. Can someone break down what each term means?
P is pressure, ρ is fluid density, g is gravitational acceleration, and z is the depth!
Exactly! And if we visualize this, it helps us understand why pressure increases with depth under gravitational fields. Any thoughts on how this principle is applied in real-world situations?
It's crucial for engineering dams or any structures needing fluid stability.
That's right! The knowledge from this concept is not only theoretical but also very practical, so keep that in mind as you study further.
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In this section, the behavior of pressure in static fluid systems is examined, especially when gravity is aligned with coordinate axes. The section covers principles such as Pascal's law, pressure gradients, and the differences between gauge and absolute pressures. It illustrates these concepts using control volume analysis and examples of hydrostatic pressure distribution.
This section explores the behavior of pressure fields in fluids at rest, focusing particularly on how gravity interacts with the coordinate axes. The discussion begins by examining the pressure field at a specific point within a stationary fluid, defined as P(x, y, z). The absence of shear stress in static fluids allows for simplifications in analysis, where Pascal's law states that pressure acts normal to a given surface.
The interplay between body forces—specifically gravitational forces—and surface pressures is critical in defining fluid behavior. The notation and use of control volumes with dimensions in the x, y, and z directions form the structural basis of the analysis, where the pressure gradient is expressed using Taylor series approximations, and its impact on forces acting along these axes is addressed.
Critical concepts discussed include the definitions of gauge pressure and absolute pressure, differentiating between them based on measurement datum (absolute zero and atmospheric pressure). The section ultimately leads to hydrostatic pressure equations that describe how pressure varies with elevation (z) in a gravitational field, elucidating the linear relationship in these scenarios. This understanding is essential for applications in fluid mechanics such as dam safety and engineering fluid systems.
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Now if I go for the next ones that how to get the pressure field when fluid is at rest. That means I am just looking the what could be the functions of the P, P = P (x, y, z). If it that it is now again I am considering a very simple case, let us consider a control volume like this okay. This is what my control volume. As I said it when the fluid is at rest the shear stress become zero. So there is no shear stress component on this fluid plane. Only this normal stress which is as equivalent to the pressure will act over this control surface.
In this chunk, we focus on determining the pressure field in a static fluid. When a fluid is at rest, it doesn't experience shear stress, meaning there's no tangential force acting at the fluid's surface. Instead, the only force acting on the control volume—a defined space we're analyzing—is the normal stress, which corresponds to the pressure. Imagine a cube of fluid suspended in space: the only thing pushing into or pulling out of this cube is pressure acting perpendicular to its surface.
Think of a balloon filled with water. When you hold the balloon still, the water inside exerts pressure outward. There's no movement or shear (like when you squish it), just the pressure from the water on the sides of the balloon. This reflects how, in a control volume at rest, only pressure needs to be considered.
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So we can have a two force components. One is the surface force component and other is body force. The body force components if you look it that it will be unit weight multiply the volume of the control volume, which is very simple things. The control volumes, the volume is this much and the unit is ρg and ρ stands for here the density and g stands for accelerations due to gravity.
Here, we identify two types of forces acting on our control volume: surface forces and body forces. Surface forces come from the pressure exerted on the sides of the control volume, while body forces are due to the weight of the fluid itself, which is calculated using the fluid's density (ρ) multiplied by gravity (g). This gives us the overall weight acting on the control volume based on its volume.
Return to the balloon; if you weigh the water inside, that weight represents the body force. However, the pressure pushing outward on the balloon's sides is akin to surface forces. Together, these two help us understand how fluids remain at rest.
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Now if you look it over this control volume, all these pressure is going to act it as Pascal law says that pressure acts normal to the surface. So that what we can consider pressures act there normal to the surface. Then we need to define now as a pressure as a x, y, z is a pressure field what we are looking it which is a function of x, y, z.
This chunk explains how pressure behaves in a control volume according to Pascal's law, which states that pressure applied to a confined fluid is transmitted undiminished in every direction. Therefore, any pressure we measure is normal (perpendicular) to the surface of the control volume and varies with position, hence being a function of x, y, and z coordinates. This means that to analyze fluid behavior, we must treat pressure as a multidimensional field.
Think about how a sponge soaks up water. As water seeps into the sponge, the pressure from that water is exerted equally in all directions. If you squeeze the sponge, you can see how the pressure builds up and acts in every direction on the sponge walls, demonstrating how pressure operates in a fluid-filled control volume.
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I can use Taylor series to approximate distance of this surface which is a far away from. The pressure at point (x,y,z) on the surface can be expressed as...
In this chunk, we discuss how to utilize a mathematical tool known as Taylor series to estimate pressure values at different points within our control volume. By taking the pressure at a known point and approximating it based on its distance from other surface points in the control volume, we can derive a more complex understanding of pressure distribution within the fluid.
Imagine you have a map of a mountain range. If you're at the peak (where you know the elevation), you can use the map to estimate the elevations (pressures) at points further down the mountain, based on how steep the slopes are. A Taylor series does something similar: it helps us estimate properties of a function based on what we already know about it at a specific point.
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If I know P(x, y, z) what will be the pressure at this point (x,y) will have this function. You can look at this negative part is there because this is what distance far away or the opposite of the y direction.
This section emphasizes the importance of maintaining equilibrium in our control volume. The pressure derived using the Taylor series helps us understand how pressure changes as we move between different points in space. This understanding allows us to establish conditions of static equilibrium, which state that the sum of forces acting in any direction must equal zero when the fluid is at rest.
Envision balancing a seesaw. If one side is heavier, it will tilt unless additional weight is added to balance it out. Similarly, for a fluid to remain still (equilibrium), the equal and opposite pressures must act across the control volume surface to maintain balance.
Learn essential terms and foundational ideas that form the basis of the topic.
Key Concepts
Pressure: The force per unit area that acts normal to a surface.
Gauge Pressure: The pressure relative to atmospheric pressure.
Hydrostatic Pressure: Pressure variation due to the weight of fluid above.
Control Volume: A finite region in space through which fluid flows, used for analysis.
See how the concepts apply in real-world scenarios to understand their practical implications.
Using a barometer to measure atmospheric pressure based on mercury levels.
Calculating gauge pressure in a tire by measuring against local atmospheric pressure.
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In fluids at rest, pressure's best, it grows with depth, forget the rest.
Imagine a calm lake. At the bottom, the weight of the water above pushes down, creating pressure that increases the deeper you go; the deeper you go, the more 'squeeze' from the weight above, hence pressure rises.
Remember 'PGA': Pressure Gradients Allow us to simplify our analysis.
Review key concepts with flashcards.
Review the Definitions for terms.
Term: Pressure
Definition:
The force exerted per unit area on a surface.
Term: Static Fluid
Definition:
A fluid that is at rest with no shear stresses acting.
Term: Gauge Pressure
Definition:
The pressure measured relative to atmospheric pressure.
Term: Absolute Pressure
Definition:
The total pressure measured from an absolute vacuum.
Term: Hydrostatic Pressure
Definition:
The pressure exerted by a fluid at rest due to the weight of the fluid above it.
Term: Control Volume
Definition:
A defined volume in which mass and energy are analyzed.