Hey, everyone! So in this video, we (re) gonna talk about Pascal's law and probably the most important application of Pascal's law, which is called the hydraulic lift. It's the basis for a lot of, like, our different hydraulic tool that we use in industrial purposes and stuff like that. Right? So let's go ahead and get started here. What Pascal's law basically says is that pressure in a confined fluid is transmitted equally throughout the fluid. Now there's a lot of words here. Basically, what this just means is if you have like a liquid that's sort of like in this weird shape like this, if you push down on one area of the tube or you apply some force here, that's gonna generate a pressure and that pressure basically gets transmitted through all of the points throughout the fluid. Alright, now how does this help us solve problems? It doesn't really, at least not yet. We got a couple more conceptual things to cover. All right. So, remember that pressure in a liquid, does or does not depend on the shape of the container. What do you guys think? Hopefully, you guys realize that it does not depend on the shape of the container. We can actually tell straight from our P bottom equation. Alright, Pbottomtop+ρgh. Now this sort of like the second point here has to do with this image. Notice how we have a bunch of different shapes, different shapes containers. And let's say I wanted to ca...
- 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 Circuits2h 7m
- 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
Pascal's Law & Hydraulic Lift - Online Tutor, Practice Problems & Exam Prep
Pascal's law states that pressure in a confined fluid is transmitted equally throughout the fluid, regardless of the container's shape. This principle is crucial in hydraulic lifts, where force is multiplied based on the ratio of cross-sectional areas (mechanical advantage). The equations and illustrate this concept, showing that pressure and volume changes are interconnected in hydraulic systems.
Pascal's Law and Hydraulic Lift
Video transcript
Hydraulic Lift / Proportional Reasoning
Video transcript
Hey guys, so let's check out this hydraulic lift example, and this is a very straightforward example. I really want to nail this point that you can solve some of these very easily if you just know the ratio between the areas. Let's check it out. So it says here, the hydraulic lift is designed with cylindrical columns, one having double the radius of the other. So, let's draw this real quick. So we've got little cylindrical columns there and one is double the radius. I'm going to call this r1 is just r, and then r2 will be 2r because it's double the radius. It says both columns are capped with pistons of the same density and thickness. That's just standard language so that you know that the pistons basically don't have an impact on anything. They cancel each other out. So it looks like that. And then it says if you push on the thinner column with the force f, so if you push with F, I'm going to say that your force F1 has a magnitude of F. How much force will act on the other piston? So how much force do you get here? Cool. And I hope you remember that the way to start this is to say, hey, the pressure on both sides is the same. So to say, p1 equals p2. Therefore, F1 equals, f1 over a1 is f2 over a2. This is because, of course, pressure is force over area. So then I can write that F2 must be F1 times (a2/a1). Now the areas here are the areas of a circle because the surface area of a cylindrical column is going to be the area of a circle, pi r squared because it is cylindrical. Cool? So this means you're going to rewrite this as πr2πr1, and I can cancel out the πs. And if you want, you can even rewrite, you can factor out the square and it's going to look like this. So it's proportional, your new force is proportional to the square of the ratio of the radii. That sounds like a mouthful, but if you have F here, which is the original force, and then the second radius is double the first, so it looks like this. 2nd radius is double the first. So the r's cancel and you're left with 22, which is 4. And we're done. The answer is 4F. Now there's a lot of math here. You could have solved this more simply by knowing that, hey, if the radius is double and the area is pi r squared, if you double the radius and the radius is squared, that means that the area is going to be 4 times greater. If the radius is doubled, the area is quadrupled and if the area is quadrupled, that means that the new force is also going to be quadrupled, or 4 times greater than the original force. Okay. Double the radius means you quadruple the area, which means you quadruple the force. You could have just done that as well. Hopefully, this serves as a little bit of a review on how to do the full solution, but you could have been that quick also. And if you remember from a previous video, I told you that if the force becomes 4 times larger, then the height difference or the height gain on the right side is going to become 4 times smaller. It's just the opposite of what happens. So if the force becomes 4 times bigger, then the height becomes 4 times smaller. That's it. Okay? That's all you need to know. Now I'm going to show how to solve this but at this point, you could have already known this but by just knowing that the amount that you're going to gain inside here is going to be smaller by the same factor that the force gets multiplied by. But let's solve this real quickly. And we solve this by knowing that the change in volume on the left, the amount of volume that goes down here is the same amount of volume that goes up here. I didn't draw that properly because I'm trying to move this quickly, but the volume on the left is the same as the volume on the right. And volume, remember, is area times height. Right? So I can write a1h1 or Δh1 because it's the change in height, equals a2Δh2. And we're looking for Δh2. So Δh2 is Δh1a1 over a2. All I've done is move the a2 to the other side of the equation and I now know that this area here this area here is 4 times larger. We know this from over here. Right? So I can just say this is Δh1, which we call just big H. And I have an area, and then I have an area that is 4 times that size. These can so and you see how you end up with H/4. Okay? That's it for this one. Let's keep going.
Force to Lift a Car
Video transcript
Hey guys, so in this hydraulic lift example, we're being asked to find the minimum force needed to lift a car. Let's check it out. Alright. So, it says the hydraulic lift is designed with cylindrical columns having these radiators here. So I'm going to draw a standard hydraulic lift. It looks something like this. The radius of the first one here, we're going to call this r1, is 20 centimeters or 0.2 meters and then this one is radius r2 is 2 meters and notice that radius r2 is 10 times larger than radius r1. Cool. And you are going to push down here with a force F1 and that's what we want to know. So that you lift a car. I'm going to draw an ugly car here. So that you can lift the car, lift car, with it. Okay. And we want to know how much force that is. Now remember, every hydraulic lift question or almost all of them are going to start with either the fact that the pressure on the left equals the pressure on the right or it's going to start with the fact that the change in volume on the left has to equal the change in volume on the right side. Okay. And because we're looking for force and force has to do with pressure, this is the equation we're going to use. Remember that pressure is force over area. So we're going to immediately, as soon as we write this, the next step is going to be to write that P1 becomes F1 over a1 and P2 becomes F2 over a2. And here we're looking for F1, the input force. I can calculate the areas because I know the radii. Right? Remember area, when you have a cylindrical column, it's going to be πr2. So if I have R, I have A, I can calculate that. What about f2? Well, f2 is the force required to lift a car. How much force do you need to lift something? The amount of force you need to lift something, you should remember this. The amount of force to lift something is the weight of that something. The weight of the object. Now you might be thinking, if I, if mg is 100 and you push with 100, isn't that just going to cancel itself out? It is. Technically, you should push with 100.0001. Right? So you have to be just barely enough. But this is kind of silly so we just set them equal to each other. Okay? But don't get confused. Don't think that just because they're equal to each other, it's not going to move. The idea is that it's slightly more than that, but we use that amount. So hopefully that makes sense. F Lift will be replaced with MG. So this right here will be MG. Okay. So now I can solve for F1 by moving a1 to the other side. So it's going to be F1 equals F2 which is mg times a1, a1 goes to the top, divided by a2. Okay. And the mass of the car is 100. Gravity, I'm going to use 10 just to make this easier. The first area, let's calculate the first area. It's going to be πr squared. I'm going to do this slowly here. And then here, πr squared. R1, r2. We're going to cancel these 2. 800 times 10 is 8,000. The first radius is 0.2 and the second radius is 2.0. Alright. So if you do this, if you do this, the best way to do 0.2 divided by 20 by the way, oop, by 2 is to multiply both sides by 10. So this becomes 2 over 20 and now you can easily see that this is just 1 over 10. Okay. Hopefully, you get that or you could just do it in a calculator. But this is going to be 8,001 divided by 10 squared. If you square the top and the bottom, you get 8,000 divided by 100. So now, 20s are going to cancel, and you're left with 80. So this is the final answer. This means that you need a force of 80 newtons. Now, check out what's happening here. If you apply a force of 80 newtons, you're gonna be able to lift this car even though it takes 8,000 newtons to lift this car. Notice that this force here is 100 times greater than your input force. And that should make sense because your radius was 10 times greater. Let me write this out. The second radius was 10 times greater than the first radius. Remember, area is πr2. So if the radius is 10 times larger, then the area is 10 square times larger. So the area is going to be 100 times larger, and therefore the force will be magnified by a factor of 100. Cool. That's it for this one. Classic example of a hydraulic lift. Let's keep going.
Do you want more practice?
More setsHere’s what students ask on this topic:
What is Pascal's Law and how does it apply to hydraulic lifts?
Pascal's Law states that pressure in a confined fluid is transmitted equally in all directions throughout the fluid, regardless of the shape of the container. This principle is fundamental in hydraulic lifts, which use a confined fluid to multiply force. In a hydraulic lift, two pistons of different cross-sectional areas are connected by a fluid-filled chamber. When a force is applied to the smaller piston, it creates pressure in the fluid, which is transmitted equally to the larger piston. The force exerted by the larger piston is greater due to its larger area, allowing heavy objects to be lifted with relatively little input force. The relationship between the forces and areas is given by the equation:
How does the shape of the container affect the pressure in a fluid according to Pascal's Law?
According to Pascal's Law, the shape of the container does not affect the pressure in a fluid. The pressure at any point in a confined fluid is determined by the height of the fluid column above that point, the density of the fluid, and the gravitational acceleration. This is expressed by the equation:
where is the pressure at a given depth, is the pressure at the top of the fluid, is the fluid density, is the gravitational acceleration, and is the depth of the fluid. Therefore, the pressure at a given depth is the same regardless of the container's shape.
What is the mechanical advantage in a hydraulic lift?
The mechanical advantage in a hydraulic lift is the factor by which the input force is multiplied to lift a heavier load. It is determined by the ratio of the cross-sectional areas of the two pistons in the hydraulic system. The mechanical advantage (MA) is given by the equation:
where is the area of the larger piston and is the area of the smaller piston. A higher mechanical advantage means that a smaller input force can lift a larger load, making hydraulic lifts highly efficient for lifting heavy objects.
How do you calculate the force exerted by a hydraulic lift?
To calculate the force exerted by a hydraulic lift, you use Pascal's Law, which states that the pressure in a confined fluid is transmitted equally in all directions. The force exerted by the larger piston (F2) can be calculated using the equation:
where F1 is the force applied to the smaller piston, A1 is the area of the smaller piston, A2 is the area of the larger piston, and F2 is the force exerted by the larger piston. Rearranging the equation to solve for F2 gives:
This equation shows that the force exerted by the larger piston is proportional to the ratio of the areas of the two pistons.
What are the key equations to remember for solving hydraulic lift problems?
When solving hydraulic lift problems, there are two key equations to remember:
1. Pressure equality:
This equation states that the pressure at the same height in a confined fluid is equal. It can be expressed as:
2. Volume conservation:
This equation states that the volume of fluid displaced by one piston must equal the volume of fluid displaced by the other piston. It can be expressed as:
These equations are essential for understanding how forces and displacements are related in hydraulic systems.
Your Physics tutor
- Hydraulic Lift II.The piston of a hydraulic automobile lift is 0.30 m in diameter. What gauge pressure, in pas...
- When a second student joins the first, the piston sinks . What is the second student's mass?
- A 55 kg cheerleader uses an oil-filled hydraulic lift to hold four 110 kg football players at a height of 1.0 ...
- A hydraulic lift is used to jack a 960-kg car 52 cm off the floor. The diameter of the output piston is 18 cm,...
- A 3.2-N force is applied to the plunger of a hypodermic needle. If the diameter of the plunger is 1.3 cm and t...
- (II) A hydraulic press for compacting powdered samples has a large cylinder which is 10.0 cm in diameter, and ...