Conceptual Physics Matter Liquids Gases

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Conceptual Physics Matter Liquids Gases Lana Sheridan De Anza College July 25, 2017

Last time atomic structure forms of matter solids density elasticity liquids & pressure

Overview liquids pressure surface tension buoyancy and Archimedes Principle Pascal s principle gases the atmosphere Boyle s law

Liquids liquid a state of matter where the constituent particles are free to move around relative to one another, but the substance is nearly incompressible. Volume is fixed, but shape is not. A solid that is heated will melt to form a liquid. If that liquid is further heated it will boil to form a gas. Both liquids and gases can flow, but the density of a substance in its liquid state is close to that in its solid state. For gases the density can vary.

Pressure Most liquids maintain nearly constant volume whatever the pressure. Pressure = Force Area P = F A Pressure is measured in Pascals, Pa; 1 Pa = 1 N/m 2. Atmospheric pressure is 101.3 kpa, or 1.013 10 5 Pa. Since the Pascal is a small unit (even 1 atmosphere is 10 5 ) sometimes atmospheres are also used as a unit of pressure. 1 atmosphere = 1.013 10 5 Pa

Pressure varies with Depth P liq = ρgh

Surface Tension The H 2 O molecules that make up water are slightly polar and attract one another. This means that water droplets tend to arrange themselves to minimize their surface area. cohesion The attraction between like molecules adhesion The attraction between molecules of different substances Water in air behaves as if it is covered with an elastic membrane because the cohesive forces between the water molecules are stronger than the adhesive forces between water and air.

Surface Tension

Mensicus A meniscus, or curvature of a liquid surface happens when a water droplet is in air, or when water is in a glass beaker. Adhesive forces between water and glass are stronger than cohesive forces within the water, so the water tends to stick to the glass. This effect can also be used to draw water up in a glass tube.

Capillary Action

Mensicus 1 https://chem.libretexts.org/core/physical and Theoretical Chemistry

Siphoning 1 Figure from Wikipedia.

Buoyancy Astronauts training in their spacesuits: The total mass of NASA s EMU (extravehicular mobility unit) is 178 kg. Why does training underwater make maneuvering in the suits easier? 1 Picture from Hubblesite.org.

Buoyancy The apparent weight of submerged objects is less than its full weight. For an object that would float, but is held underwater, its apparent weight is negative! There is an upward force on an object in a fluid called the buoyant force.

Buoyancy and Archimedes Principle Archimedes Principle The buoyant force on an object is equal to the weight of the fluid that the object displaces. F buoy = W df Logically, if a brick falls to the bottom of a pool it must push an amount water equal to its volume up and out of the way.

Buoyancy and Archimedes Principle For a fully submerged object the weight of the displaced fluid is the product of the density of the fluid, ρ f, the volume of the object, V obj, and g, so: F buoy = ρ f V obj g ρ f V obj is the mass of the water moved aside by the object.

Buoyancy and Archimedes Principle An object that floats will displace less fluid than its entire volume. For a floating object: F buoy = ρ f V sub g where V sub is the volume of the part of the object underneath the fluid level only.

Sinking and Floating Will a particular object sink or float in a particular fluid? If the object is less dense than the fluid it will float. If the object is more dense than the fluid it will sink. If the object and the fluid have the same density if will neither float or sink, but drift at equilibrium.

Sinking and Floating A floating object displaces a mass of water equal to its own mass! (Equivalently, a weight of water equal to its own weight.) This also means that ρ f V sub = m obj. Whether it sinks or floats, always: F buoy = W df

Questions Military ships are often compared by their displacements, the weight (or mass, depending on context) of water they displace. The USS Enterprise was an aircraft carrier (now decommissioned). Displacement: 94,781 tonnes (metric tons), fully loaded. 1 tonne = 1000 kg What is the mass of the fully loaded USS Enterprise in kgs?

Questions Military ships are often compared by their displacements, the weight (or mass, depending on context) of water they displace. The USS Enterprise was an aircraft carrier (now decommissioned). Displacement: 94,781 tonnes (metric tons), fully loaded. 1 tonne = 1000 kg What is the mass of the fully loaded USS Enterprise in kgs? Ans: 94,781,000 kg

Questions Military ships are often compared by their displacements, the weight (or mass, depending on context) of water they displace. The USS Enterprise was an aircraft carrier (now decommissioned). Displacement: 94,781 tonnes (metric tons), fully loaded. 1 tonne = 1000 kg What is the mass of the fully loaded USS Enterprise in kgs? Ans: 94,781,000 kg Problem # 8, page 246. Your friend of mass 100 kg can just barely float in fresh water. Calculate her approximate volume.

Questions Military ships are often compared by their displacements, the weight (or mass, depending on context) of water they displace. The USS Enterprise was an aircraft carrier (now decommissioned). Displacement: 94,781 tonnes (metric tons), fully loaded. 1 tonne = 1000 kg What is the mass of the fully loaded USS Enterprise in kgs? Ans: 94,781,000 kg Problem # 8, page 246. Your friend of mass 100 kg can just barely float in fresh water. Calculate her approximate volume. Ans: 0.1 m 3

Pascal s Principle (Or, how hydraulic systems work.) Liquids are (mostly) incompressible. If you push on a piston at one end of a pipe you will move the liquid at the far end. Pascal s Principle A change in pressure at any point in an enclosed fluid at rest is transmitted undiminished to all points in the fluid.

Pascal s Principle Since the pressures at the left end and the right end are the same: Since A 2 > A 1, F 2 > F 1. P 1 = P 2 F 1 = F 2 A 1 A 2

Pascal s Principle This has applications: 1 Figure from hyperphysics.phy-astr.gsu.edu.

Question If a pair of pistons are connected on either end of a hydraulic tube. The first has area 0.2 m 2 and the second has an area of 4 m 2. A force of 30 N is applied the first piston. What is the force exerted by the second piston on a mass that rests on it?

Question If a pair of pistons are connected on either end of a hydraulic tube. The first has area 0.2 m 2 and the second has an area of 4 m 2. A force of 30 N is applied the first piston. What is the force exerted by the second piston on a mass that rests on it? Ans: F 2 = 600 N

Question If a pair of pistons are connected on either end of a hydraulic tube. The first has area 0.2 m 2 and the second has an area of 4 m 2. A force of 30 N is applied the first piston. What is the force exerted by the second piston on a mass that rests on it? Ans: F 2 = 600 N If the first piston is depressed a distance of 1 m by the 30 N force, how far does the second piston rise?

Question If a pair of pistons are connected on either end of a hydraulic tube. The first has area 0.2 m 2 and the second has an area of 4 m 2. A force of 30 N is applied the first piston. What is the force exerted by the second piston on a mass that rests on it? Ans: F 2 = 600 N If the first piston is depressed a distance of 1 m by the 30 N force, how far does the second piston rise? Ans: 0.05m = 5cm

Gases gas a state of matter where the constituent particles are vastly separated from one another and free to move around. A liquid that is heated will boil to form a gas. A gas heated much further will form a plasma. Both liquids and gases can flow, but the density of gases can vary and they are readily compressible. The large distances between individual molecules or atoms is why most gases are transparent.

Elemental Gases hydrogen (H 2 ), nitrogen (N 2 ) oxygen (O 2 ) fluorine (F 2 ) chlorine (Cl 2 ) helium (He) neon (Ne) argon (Ar) krypton (Kr) xenon (Xe) radon (Rn)

The Atmosphere We are living in a sea of air. It is held in place by Earth s gravity and made up of: nitrogen, N 2, 78% oxygen, O 2, 21% argon, Ar, 1% carbon dioxide, CO 2, 0.4% It also contains less that 1% water vapor.

Layers of the Atmosphere 1 Picture shot from the ISS, courtesy of NASA Earth Observatory.

Air Pressure Just like liquids, gases also exert pressure on their surroundings. Atmospheric pressure at sea level is 101.3 kpa. Atmospheric pressure falls with increasing altitude. Atmospheric pressure fluctuates locally from place to place, day to day.

Barometers Barometers are devices for measuring local atmospheric pressure. Typically, simple barometers are filled with mercury, which is very dense. The weight of the mercury in the tube exerts the same pressure as the surrounding atmosphere. On low pressure days, the level of the mercury drops. On high pressure days it rises.

Boyle s Law Suppose you seal a fixed mass of gas in a container. If you compress it, you will decrease the volume, but increase the pressure. If you let it expand, you increase the volume but decrease the pressure. For a fixed mass of gas at a constant temperature: P 1 V 1 = P 2 V 2 This is Boyle s Law.

Summary liquids pressure surface tension buoyancy Pascal s principle gases the atmosphere Talks! Aug 8-9. Homework Hewitt, Ch 13, onward from page 243. Exercises: 15, 25; Problems: 3, 5, 7 Ch 14, onward from page 262. Ranking 1; Exercises: 9, 17, 19, 40, 47, (53); Problems: 1