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Lect 7.ppt

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Course of lectures «Contemporary Physics: Part1»Lecture №7Temperature.Heat and the First Law of Thermodynamics.

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Слайд 1Quick Quiz 4.1 Suppose you are standing directly behind someone

who steps back and accidentally stomps on your foot with

the heel of one shoe. Would you be better off if that person were (a) a large professional basketball player wearing sneakers (b) a petite woman wearing spike-heeled shoes?

Quick Quiz 4.2 A grandfather clock depends on the period of a pendulum to keep correct time. Suppose a grandfather clock is calibrated correctly and then a mischievous child slides the bob of the pendulum downward on the oscillating rod. Does the grandfather clock run (a) slow (b) fast (c) correctly?

Quick Quiz 4.1 Suppose you are standing directly behind someone who steps back and accidentally stomps on

Слайд 2Course of lectures «Contemporary Physics: Part1»
Lecture №7

Temperature.
Heat and the First

Law of Thermodynamics.

Course of lectures «Contemporary Physics: Part1»Lecture №7Temperature.Heat and the First Law of Thermodynamics.

Слайд 3We now direct our attention to the study of thermodynamics,

which involves situations in which the temperature or state (solid,

liquid, gas) of a system changes due to energy transfers. As we shall see, thermodynamics is very successful in explaining the bulk properties of matter and the correlation between these properties and the mechanics of atoms and molecules.
We now direct our attention to the study of thermodynamics, which involves situations in which the temperature

Слайд 4Temperature and the Zeroth
Law of Thermodynamics
For purposes of the current

discussion, we assume that two objects are in thermal contact

with each other if energy can be exchanged between them by these processes due to a temperature difference.

Thermal equilibrium is a situation in which two objects would not exchange energy by heat or electromagnetic radiation if they were placed in thermal contact.

Temperature and the ZerothLaw of ThermodynamicsFor purposes of the current discussion, we assume that two objects are

Слайд 5Temperature and the Zeroth
Law of Thermodynamics
Figure 19.1 The zeroth law

of thermodynamics. (a) and (b) If the temperatures of A

and B are measured to be the same by placing them in thermal contact with a thermometer (object C), no energy will be exchanged between them when they are placed in thermal contact with each other (c).
Temperature and the ZerothLaw of ThermodynamicsFigure 19.1 The zeroth law of thermodynamics. (a) and (b) If the

Слайд 6We can summarize these results in a statement known as

the zeroth law of thermodynamics (the law of equilibrium):
Temperature and

the Zeroth
Law of Thermodynamics

If objects A and B are separately in thermal equilibrium with a third object C, then A and B are in thermal equilibrium with each other.

We can summarize these results in a statement known as the zeroth law of thermodynamics (the law

Слайд 7Thermometers and the Celsius
Temperature Scale
As a result of thermal expansion,

the level of the mercury in the thermometer rises as

the mercury is heated by water in the test tube.
Thermometers and the CelsiusTemperature ScaleAs a result of thermal expansion, the level of the mercury in the

Слайд 8The Constant-Volume Gas Thermometer
and the Absolute Temperature Scale
A constant-volume gas

thermometer measures the pressure of the gas contained in the

flask immersed in the bath. The volume of gas in the flask is kept constant by raising or lowering reservoir B to keep the mercury level in column A constant.
The Constant-Volume Gas Thermometerand the Absolute Temperature ScaleA constant-volume gas thermometer measures the pressure of the gas

Слайд 9The Constant-Volume Gas Thermometer
and the Absolute Temperature Scale
A typical graph

of pressure versus temperature taken with a constant-volume gas thermometer.

The two dots represent known reference temperatures (the ice and steam points of water).
The Constant-Volume Gas Thermometerand the Absolute Temperature ScaleA typical graph of pressure versus temperature taken with a

Слайд 10The Constant-Volume Gas Thermometer
and the Absolute Temperature Scale
Pressure versus temperature

for experimental trials in which gases have different pressures in

a constant-volume gas thermometer. Note that, for all three trials, the pressure extrapolates to zero at the temperature -273.15°C.
The Constant-Volume Gas Thermometerand the Absolute Temperature ScalePressure versus temperature for experimental trials in which gases have

Слайд 11Thermal Expansion of Solids
and Liquids
Thermal expansion is a consequence

of the change in the average separation between the atoms

in an object.
Thermal Expansion of Solids and LiquidsThermal expansion is a consequence of the change in the average separation

Слайд 12Thermal Expansion of Solids
and Liquids
average coefficient of linear expansion
(9.1)
(9.2)
A

cavity in a piece of material expands in the same

way as if the cavity were filled with the material.
Thermal Expansion of Solids and Liquidsaverage coefficient of linear expansion(9.1)(9.2)A cavity in a piece of material expands

Слайд 13Thermal Expansion of Solids
and Liquids
Table 9.1

Thermal Expansion of Solids and LiquidsTable 9.1

Слайд 14Thermal Expansion of Solids
and Liquids
β is the average coefficient

of volume expansion.
(9.3)

Thermal Expansion of Solids and Liquidsβ is the average coefficient of volume expansion.(9.3)

Слайд 15Thermal Expansion of Solids
and Liquids

Thermal Expansion of Solids and Liquids

Слайд 16Thermal Expansion of Solids
and Liquids
Figure 9.1 (a) A bimetallic

strip bends as the temperature changes because the two metals

have different expansion coefficients. (b) A bimetallic strip used in a thermostat to break or make electrical contact.
Thermal Expansion of Solids and LiquidsFigure 9.1 (a) A bimetallic strip bends as the temperature changes because

Слайд 17The Unusual Behavior of Water
Figure 9.2 The variation in the

density of water at atmospheric pressure with temperature. The inset

at the right shows that the maximum density of water occurs at 4°C.
The Unusual Behavior of WaterFigure 9.2 The variation in the density of water at atmospheric pressure with

Слайд 18Macroscopic Description of an Ideal Gas
It is convenient to express

the amount of gas in a given volume in terms

of the number of moles n. One mole of any substance is that amount of the substance that contains Avogadro’s number NA = 6.022 ) 1023 of constituent particles (atoms or molecules).

(9.4)

Macroscopic Description of an Ideal GasIt is convenient to express the amount of gas in a given

Слайд 19Macroscopic Description of an Ideal Gas
(9.5)
Equation of state for an

ideal gas

Macroscopic Description of an Ideal Gas(9.5)Equation of state for an ideal gas

Слайд 20Macroscopic Description of an Ideal Gas
Figure 9.4 A bottle of

champagne is shaken and opened. Liquid spews out of the

opening. A common misconception is that the pressure inside the bottle is increased due to the shaking.
Macroscopic Description of an Ideal GasFigure 9.4 A bottle of champagne is shaken and opened. Liquid spews

Слайд 21Macroscopic Description of an Ideal Gas
(9.6)

Macroscopic Description of an Ideal Gas(9.6)

Слайд 22Heat and Internal Energy
Internal energy is all the energy of

a system that is associated with its microscopic components—atoms and

molecules—when viewed from a reference frame at rest with respect to the center of mass of the system.

Heat is defined as the transfer of energy across the boundary of a system due to a temperature difference between the system and its surroundings.

Heat and Internal EnergyInternal energy is all the energy of a system that is associated with its

Слайд 23Units of Heat
An energy unit related to thermal processes, the

calorie (cal), which is defined as the amount of energy

transfer necessary to raise the temperature of 1 g of water from 14.5°C to 15.5°C. (Note that the “Calorie,” written with a capital “C” and used in describing the energy content of foods, is actually a kilocalorie.) The unit of energy in the U.S. customary system is the British thermal unit (Btu), which is defined as the amount of energy transfer required to raise the temperature of 1 lb of water from 63°F to 64°F.
Scientists are increasingly using the SI unit of energy, the joule, when describing thermal processes.
Units of Heat	An energy unit related to thermal processes, the calorie (cal), which is defined as the

Слайд 24The Mechanical Equivalent of Heat
(9.7)
Figure 9.5 Joule’s experiment for determining

the mechanical equivalent of heat. The falling blocks rotate the

paddles, causing the temperature of the water to increase.
The Mechanical Equivalent of Heat(9.7)Figure 9.5 Joule’s experiment for determining the mechanical equivalent of heat. The falling

Слайд 25Specific Heat and Calorimetry
The heat capacity C of a particular

sample of a substance is defined as the amount of

energy needed to raise the temperature of that sample by 1°C.

The specific heat c of a substance is the heat capacity per unit mass.

(9.8)

(9.9)

Specific Heat and CalorimetryThe heat capacity C of a particular sample of a substance is defined as

Слайд 26Specific Heat and Calorimetry
From this definition, we can relate the

energy Q transferred between a sample of mass m of

a material and its surroundings to a temperature change ∆T as

(9.10)

Specific Heat and CalorimetryFrom this definition, we can relate the energy Q transferred between a sample of

Слайд 27Specific Heat and Calorimetry

Specific Heat and Calorimetry

Слайд 28Conservation of Energy: Calorimetry
(9.11)

Conservation of Energy: Calorimetry(9.11)

Слайд 29Latent Heat
From the definition of latent heat, and again choosing

heat as our energy transfer mechanism, we find that the

energy required to change the phase of a given mass m of a pure substance is

(9.12)

Latent heat of fusion Lf is the term used when the phase change is from solid to liquid (to fuse means “to combine by melting”), and latent heat of vaporization Lv is the term used when the phase change is from liquid to gas (the liquid “vaporizes”).

Latent HeatFrom the definition of latent heat, and again choosing heat as our energy transfer mechanism, we

Слайд 30Latent Heat

Latent Heat

Слайд 31Work and Heat in Thermodynamic Processes
Figure 9.6 Work is done

on a gas contained in a cylinder at a pressure

P as the piston is pushed downward so that the gas is compressed.

(9.13)

(9.14)

Work and Heat in Thermodynamic ProcessesFigure 9.6 Work is done on a gas contained in a cylinder

Слайд 32Work and Heat in Thermodynamic Processes
Figure 9.7 A gas is

compressed quasi-statically (slowly) from state i to state f. The

work done on the gas equals the negative of the area under the PV curve.

The work done on a gas in a quasi-static process that takes the gas from an initial state to a final state is the negative of the area under the curve on a PV diagram, evaluated between the initial and final states.

Work and Heat in Thermodynamic ProcessesFigure 9.7 A gas is compressed quasi-statically (slowly) from state i to

Слайд 33Work and Heat in Thermodynamic Processes
Figure 9.8 The work done

on a gas as it is taken from an initial

state to a final state depends on the path between these states.
Work and Heat in Thermodynamic ProcessesFigure 9.8 The work done on a gas as it is taken

Слайд 34Work and Heat in Thermodynamic Processes
Energy transfer by heat, like

work done, depends on the initial, final, and intermediate states

of the system.

Figure 9.9 (a) A gas at temperature Ti expands slowly while absorbing energy from a reservoir in order to maintain a constant temperature. (b) A gas expands rapidly into an evacuated region after a membrane is broken.

Work and Heat in Thermodynamic ProcessesEnergy transfer by heat, like work done, depends on the initial, final,

Слайд 35The First Law of Thermodynamics
the change in the internal energy

of the system,
independent of the path.
the internal energy
the change

in internal energy

The first law of thermodynamics

(9.15)

The First Law of Thermodynamicsthe change in the internal energy of the system, independent of the path.the

Слайд 36The First Law of Thermodynamics
First, consider an isolated system—that is,

one that does not interact with its surroundings.
The internal energy

Eint of an isolated system remains constant.
The First Law of ThermodynamicsFirst, consider an isolated system—that is, one that does not interact with its

Слайд 37The First Law of Thermodynamics
Next, consider the case of a

system (one not isolated from its surroundings) that is taken

through a cyclic process—that is, a process that starts and ends at the same state.

In a cyclic process, the net work done on the system per cycle equals the area enclosed by the path representing the process on a PV diagram.

The First Law of ThermodynamicsNext, consider the case of a system (one not isolated from its surroundings)

Слайд 38Quick Quiz 5.1

Two objects, with different sizes, masses, and

temperatures, are placed in thermal contact. Energy travels (a) from

the larger object to the smaller object (b) from the object with more mass to the one with less (c) from the object at higher temperature to the object at lower temperature.
Quick Quiz 5.1 Two objects, with different sizes, masses, and temperatures, are placed in thermal contact. Energy

Слайд 39Quick Quiz 5.2

Consider the following pairs of materials. Which

pair represents two materials, one of which is twice as

hot as the other? (a) boiling water at 100°C, a glass of water at 50°C (b) boiling water at 100°C, frozen methane at -50°C (c) an ice cube at -20°C, flames from a circus fire-eater at 233°C (d) No pair represents materials one of which is twice as hot as the other
Quick Quiz 5.2 Consider the following pairs of materials. Which pair represents two materials, one of which

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