Hey, everyone. So in this problem, we're going to cover a type of pressure gauge used to calculate pressure, called a U-shaped tube or sometimes it's called a U tube. So let's check this out here. This is going to be a pretty long video, but there's some really important information here. So let's check this out. Remember, all pressure gauges use height differences to calculate pressure. And just like always, we're going to use our pressure equation, pbottom=ptop+ρgh. Alright, so this is basically what a U tube shape looks like, or a U-shaped tube literally looks exactly like how it sounds. It's a U-shaped tube that could be open on both sides or could be opened on one side and closed on the other. Alright, let's look at the first couple of cases here, which are relatively straightforward. If you had this open end on both sides, so if you have air basically and it's open over here, then what happens is, if you fill this thing with one liquid, like let's say water or something, it's basically just going to seek to level itself out like this. Because these things are both touching air, they're going to be at the same pressure and they're going to have the same height because it's the same liquid. Right? So that's really straightforward. There's nothing new there. It's actually pretty trivial. The second one is where you have one liquid end where you have a vacuum on one side. The only way you can get a vacuum is where you close off one of the ends like this. So what happens here is, if you were to fill some liquid inside, what happens is, it's going to level off here. But then, over here, what do you think is going to happen? Is the level going to be higher or lower than this point over here? Hopefully, you guys realize it’s actually going to be higher like this. And the reason for that is that if you have air that is pushing down on this with presumably, let's say, standard atmospheric pressure, then basically what happens is if the water level is like this, you're going to push down more with one atmosphere because there's no pressure over here. If you have a vacuum, this pressure is going to be zero. And so therefore, what happens is it's going to sort of lopside like that. Alright? So you're basically just going to have that this column here is going to go up. Alright? So, that's pretty straightforward. Now let's take a look at when things get a little bit interesting. Alright. So these sort of both cases were kind of trivial in the sense that, you know, there's not really a whole lot of new physics going on there. But the most sort of common case in most of your problems is going to involve when you have two liquids and both the sides are open and you're going to dump one liquid into one side. Here's what I mean by this. So let's say you have one liquid over here. I'm going to call this blue like this. Right. And you're going to take another liquid of a different density, so I'm going to have this is going to be ρ1, and I'm going to have another liquid that I'm going to sort of drop in here like this. Right? So I'm going to fill this whole thing up with like a little column like that. Now because this thing is going to be extra weight on the right side, it's going to want to push down and it's going to try to level itself out. Now what's really important here is that it's not going to level out in such a way that it's basically going to get even again because what happens is you now have two different densities. Remember, you're going to have the same liquid at the same height equal to the same pressure, but these two things, if they're different densities, they're not going to have, it's not going to be the same liquid, so they're not going to try to level themselves out. Instead, what's going to happen is that the right column is going to push down just a little bit, and then it's going to find sort of like its new balance like this. So it's going to sit and it's going to rest on top and basically, we're going to have this little rectangle like this. Right? So this is going to be your second liquid on the right side. Now, what happens is you've displaced this amount of water, so that's going to have to appear on the left side. You're going to have to go basically up by the same amounts, roughly over here. And so basically, this is going to be where the new water level is. That's all the water that you've added by displacing from the right side. Now, what happens is there are four really important points in these U-shaped tubes. So I kind of want to go over them really quickly here. The first thing is that you want to call the left side one because that's where all the left liquid is. I'm going to call this one here the second one on the right side. Alright. So there are a couple of important points here. The first is going to be where the top of the left column finally ends up when it's finished. I'm going to call that point A. The second point here is actually going to be the points where if you draw it all the way across, it's basically going to be where the boundary of the two liquids are. So this point right here, I'm going to call this point B. And if you go all the way across, this point here is going to be point D. Alright. And at this point, which is the top of where the right column finally ends up, is going to be point C. Alright. So there are a couple of important distances to sort of note here, which that this distance is going to be. I'm going to call this h1 and this distance here is going to be h2. Alright. So the height of the actual column itself is not going to be equal to the amount of water that it displaces. And again, it's because these things are different densities. Alright. So, what happens here is there's another height, which is going to be basically where the top of the right column is relative to the top of the left column. So it's basically just like the difference in the heights between the right and left columns. Because it's a difference in heights, I'm going to call this Δh like this. And what we can see here from this diagram is that these two things sort of are the same level like this, then that means that Δh just has to be the difference between h2 and h1. So just to put some numbers real quick, imagine this was 10 and imagine that this was 7, then this would have to be Δh3. Right? That's kind of just an important equation. Alright. So in other words, the first equation that we're going to have for these U-shaped tubes is that Δh, the difference in height, is really just going to be the height of the second column minus the height of the first. Right? So it's going to be the difference between the two column heights like this. Now what happens is in some problems, this actually could go lower and you could have the left side go on top. So in order just to make all the units positive in order to get everything positive and not get any weird negative numbers, you just stick an absolute value sign in there."
- 0. Math Review31m
- 1. Intro to Physics Units1h 23m
- 2. 1D Motion / Kinematics3h 56m
- Vectors, Scalars, & Displacement13m
- Average Velocity32m
- Intro to Acceleration7m
- Position-Time Graphs & Velocity26m
- Conceptual Problems with Position-Time Graphs22m
- Velocity-Time Graphs & Acceleration5m
- Calculating Displacement from Velocity-Time Graphs15m
- Conceptual Problems with Velocity-Time Graphs10m
- Calculating Change in Velocity from Acceleration-Time Graphs10m
- Graphing Position, Velocity, and Acceleration Graphs11m
- Kinematics Equations37m
- Vertical Motion and Free Fall19m
- Catch/Overtake Problems23m
- 3. Vectors2h 43m
- Review of Vectors vs. Scalars1m
- Introduction to Vectors7m
- Adding Vectors Graphically22m
- Vector Composition & Decomposition11m
- Adding Vectors by Components13m
- Trig Review24m
- Unit Vectors15m
- Introduction to Dot Product (Scalar Product)12m
- Calculating Dot Product Using Components12m
- Intro to Cross Product (Vector Product)23m
- Calculating Cross Product Using Components17m
- 4. 2D Kinematics1h 42m
- 5. Projectile Motion3h 6m
- 6. Intro to Forces (Dynamics)3h 22m
- 7. Friction, Inclines, Systems2h 44m
- 8. Centripetal Forces & Gravitation7h 26m
- Uniform Circular Motion7m
- Period and Frequency in Uniform Circular Motion20m
- Centripetal Forces15m
- Vertical Centripetal Forces10m
- Flat Curves9m
- Banked Curves10m
- Newton's Law of Gravity30m
- Gravitational Forces in 2D25m
- Acceleration Due to Gravity13m
- Satellite Motion: Intro5m
- Satellite Motion: Speed & Period35m
- Geosynchronous Orbits15m
- Overview of Kepler's Laws5m
- Kepler's First Law11m
- Kepler's Third Law16m
- Kepler's Third Law for Elliptical Orbits15m
- Gravitational Potential Energy21m
- Gravitational Potential Energy for Systems of Masses17m
- Escape Velocity21m
- Energy of Circular Orbits23m
- Energy of Elliptical Orbits36m
- Black Holes16m
- Gravitational Force Inside the Earth13m
- Mass Distribution with Calculus45m
- 9. Work & Energy1h 59m
- 10. Conservation of Energy2h 51m
- Intro to Energy Types3m
- Gravitational Potential Energy10m
- Intro to Conservation of Energy29m
- Energy with Non-Conservative Forces20m
- Springs & Elastic Potential Energy19m
- Solving Projectile Motion Using Energy13m
- Motion Along Curved Paths4m
- Rollercoaster Problems13m
- Pendulum Problems13m
- Energy in Connected Objects (Systems)24m
- Force & Potential Energy18m
- 11. Momentum & Impulse3h 40m
- Intro to Momentum11m
- Intro to Impulse14m
- Impulse with Variable Forces12m
- Intro to Conservation of Momentum17m
- Push-Away Problems19m
- Types of Collisions4m
- Completely Inelastic Collisions28m
- Adding Mass to a Moving System8m
- Collisions & Motion (Momentum & Energy)26m
- Ballistic Pendulum14m
- Collisions with Springs13m
- Elastic Collisions24m
- How to Identify the Type of Collision9m
- Intro to Center of Mass15m
- 12. Rotational Kinematics2h 59m
- 13. Rotational Inertia & Energy7h 4m
- More Conservation of Energy Problems54m
- Conservation of Energy in Rolling Motion45m
- Parallel Axis Theorem13m
- Intro to Moment of Inertia28m
- Moment of Inertia via Integration18m
- Moment of Inertia of Systems23m
- Moment of Inertia & Mass Distribution10m
- Intro to Rotational Kinetic Energy16m
- Energy of Rolling Motion18m
- Types of Motion & Energy24m
- Conservation of Energy with Rotation35m
- Torque with Kinematic Equations56m
- Rotational Dynamics with Two Motions50m
- Rotational Dynamics of Rolling Motion27m
- 14. Torque & Rotational Dynamics2h 5m
- 15. Rotational Equilibrium3h 39m
- 16. Angular Momentum3h 6m
- Opening/Closing Arms on Rotating Stool18m
- Conservation of Angular Momentum46m
- Angular Momentum & Newton's Second Law10m
- Intro to Angular Collisions15m
- Jumping Into/Out of Moving Disc23m
- Spinning on String of Variable Length20m
- Angular Collisions with Linear Motion8m
- Intro to Angular Momentum15m
- Angular Momentum of a Point Mass21m
- Angular Momentum of Objects in Linear Motion7m
- 17. Periodic Motion2h 9m
- 18. Waves & Sound3h 40m
- Intro to Waves11m
- Velocity of Transverse Waves21m
- Velocity of Longitudinal Waves11m
- Wave Functions31m
- Phase Constant14m
- Average Power of Waves on Strings10m
- Wave Intensity19m
- Sound Intensity13m
- Wave Interference8m
- Superposition of Wave Functions3m
- Standing Waves30m
- Standing Wave Functions14m
- Standing Sound Waves12m
- Beats8m
- The Doppler Effect7m
- 19. Fluid Mechanics2h 27m
- 20. Heat and Temperature3h 7m
- Temperature16m
- Linear Thermal Expansion14m
- Volume Thermal Expansion14m
- Moles and Avogadro's Number14m
- Specific Heat & Temperature Changes12m
- Latent Heat & Phase Changes16m
- Intro to Calorimetry21m
- Calorimetry with Temperature and Phase Changes15m
- Advanced Calorimetry: Equilibrium Temperature with Phase Changes9m
- Phase Diagrams, Triple Points and Critical Points6m
- Heat Transfer44m
- 21. Kinetic Theory of Ideal Gases1h 50m
- 22. The First Law of Thermodynamics1h 26m
- 23. The Second Law of Thermodynamics3h 11m
- 24. Electric Force & Field; Gauss' Law3h 42m
- 25. Electric Potential1h 51m
- 26. Capacitors & Dielectrics2h 2m
- 27. Resistors & DC Circuits3h 8m
- 28. Magnetic Fields and Forces2h 23m
- 29. Sources of Magnetic Field2h 30m
- Magnetic Field Produced by Moving Charges10m
- Magnetic Field Produced by Straight Currents27m
- Magnetic Force Between Parallel Currents12m
- Magnetic Force Between Two Moving Charges9m
- Magnetic Field Produced by Loops and Solenoids42m
- Toroidal Solenoids aka Toroids12m
- Biot-Savart Law (Calculus)18m
- Ampere's Law (Calculus)17m
- 30. Induction and Inductance3h 37m
- 31. Alternating Current2h 37m
- Alternating Voltages and Currents18m
- RMS Current and Voltage9m
- Phasors20m
- Resistors in AC Circuits9m
- Phasors for Resistors7m
- Capacitors in AC Circuits16m
- Phasors for Capacitors8m
- Inductors in AC Circuits13m
- Phasors for Inductors7m
- Impedance in AC Circuits18m
- Series LRC Circuits11m
- Resonance in Series LRC Circuits10m
- Power in AC Circuits5m
- 32. Electromagnetic Waves2h 14m
- 33. Geometric Optics2h 57m
- 34. Wave Optics1h 15m
- 35. Special Relativity2h 10m
Pressure Gauge: U-shaped Tube - Online Tutor, Practice Problems & Exam Prep
U-shaped tubes, or U-tubes, are essential for measuring pressure differences using height variations of liquids. The fundamental equation is . When two liquids of different densities are involved, the heights adjust to maintain equilibrium, leading to the equation . Understanding these principles is crucial for solving related problems in fluid mechanics.
Pressure Gauges: U-Shaped Tube
Video transcript
Water and oil are poured into a u-shape tube, as shown below. The column of oil, on the right side, is 25 cm tall, and the distance between the top of the two columns is 9 cm. Calculate the density of the oil.
360 kg/m3
560 kg/m3
640 kg/m3
1562 kg/m3
Do you want more practice?
More setsHere’s what students ask on this topic:
What is a U-shaped tube and how is it used to measure pressure?
A U-shaped tube, or U-tube, is a device used to measure pressure differences by observing the height variations of liquids within the tube. It consists of a U-shaped glass tube that can be open on both ends or closed on one end. When a liquid is added, the height of the liquid columns adjusts to balance the pressure. The fundamental equation used is , where is the liquid density, is the acceleration due to gravity, and is the height difference. This setup allows for the calculation of pressure differences between two points.
How do you calculate the pressure difference in a U-shaped tube with two different liquids?
To calculate the pressure difference in a U-shaped tube with two different liquids, you use the equation . Here, and are the densities of the two liquids, and and are the heights of the liquid columns. This equation ensures that the pressure at the interface of the two liquids is balanced. By knowing the densities and measuring the heights, you can determine the pressure difference between the two sides of the tube.
What is the significance of the height difference in a U-shaped tube?
The height difference in a U-shaped tube is crucial for determining the pressure difference between two points. This difference, denoted as , is calculated using the equation . The height difference directly relates to the pressure difference via the equation . In cases with two different liquids, the height difference helps in balancing the pressures at the interface, ensuring equilibrium. This principle is fundamental in fluid mechanics and is widely used in various applications, including manometers and barometers.
How do you derive the equation ρ₁h₁ = ρ₂h₂ for a U-shaped tube?
To derive the equation for a U-shaped tube, start with the pressure balance at the interface of the two liquids. The pressure at the bottom of the left column is , and the pressure at the bottom of the right column is . Since the pressures at the same height in the same liquid are equal, . Setting the right sides of these equations equal and canceling out common terms, you get .
What are the common applications of U-shaped tubes in real life?
U-shaped tubes are commonly used in various applications to measure pressure differences. One of the primary uses is in manometers, which measure the pressure of gases or liquids. They are also used in barometers to measure atmospheric pressure. In laboratory settings, U-tubes help in experiments involving fluid dynamics and pressure measurements. Additionally, they are used in HVAC systems to measure the pressure drop across filters and other components. The simplicity and accuracy of U-shaped tubes make them valuable tools in both educational and industrial contexts.