Test 1 Flashcards

1
Q

Conservation of energy principle

A

states that during an interaction, energy can change from one form to another but the total amount of energy remains constant. That is, energy cannot be created or destroyed (see first law of thermodynamics).

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2
Q

First law of thermodynamics

A

is simply a statement of the conservation of energy principle, and it asserts that total energy is a thermodynamic property. Joule’s experiments indicate the following: For all adiabatic processes between two specified states of a closed system, the net work done is the same regardless of the nature of the closed system and the details of the process. It may be expressed as follows: Energy can be neither created nor destroyed; it can only change forms. The net change (increase or decrease) in the total energy of the system during a process is equal to the difference between the total energy entering and the total energy leaving the system during that process.

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3
Q

Second law of thermodynamics

A

(increase of entropy principle) is expressed as the entropy of an isolated system during a process always increases or, in the limiting case of a reversible process, remains constant. In other words, the entropy of an isolated system never decreases. It also asserts that energy has quality as well as quantity, and actual processes occur in the direction of decreasing quality of energy.

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4
Q

Classical thermodynamics

A

is the macroscopic approach to the study of thermodynamics that does not require knowledge of the behavior of individual particles.

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5
Q

Statistical thermodynamics

A

is an approach to thermodynamics more elaborate than classical thermodynamics, based on the average behavior of large groups of individual particles.

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6
Q

Dimensions

A

are any physical characterizations of a quantity

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7
Q

Units

A

are the arbitrary magnitudes assigned to the dimensions.

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8
Q

Primary or fundamental dimensions

A

such as mass m, length L, time t, and temperature T, are the basis for the derivation of secondary dimensions.

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9
Q

Secondary or derived dimensions

A

such as velocity V, energy E, and volume V, are expressed in terms of the primary dimensions

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10
Q

English system

A

which is also known as the United States Customary System (USCS), has the respective units the pound-mass (lbm), foot (ft), and second (s). The pound symbol lb is actually the abbreviation of libra, which was the ancient Roman unit of weight.

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11
Q

Metric SI

A

(from Le Système International d’ Unités), which is also known as the International System, is based on six fundamental dimensions. Their units, adopted in 1954 at the Tenth General Conference of Weights and Measures, are: meter (m) for length, kilogram (kg) for mass, second (s) for time, ampere (A) for electric current, degree Kelvin (K) for temperature, candela (cd) for luminous intensity (amount of light), and mole (mol) for the amount of matter.

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12
Q

Joule

A

(J) is a unit of energy and has the unit “newton-meter (N·m).”

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13
Q

Btu (British thermal unit)

A

is the energy unit in the English system needed to raise the temperature of 1 lbm of water at 68°F by 1°F.

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14
Q

Calorie

A

(cal) is the amount of energy in the metric system needed to raise the temperature of 1 g of water at 15°C by 1°C.

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15
Q

Watt

A

(W) is a unit that is equivalent to joule per second (J/s).

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16
Q

Secondary units

A

are expressed in terms of the primary units.

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17
Q

Unity conversion ratios

A

are ratios of units that are based on the definitions of the units in question that are identically equal to 1, are unitless, and can be inserted into any calculation to properly convert units.

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18
Q

Surroundings

A

are everything outside the system boundaries.

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19
Q

Boundary

A

is the real or imaginary surface that separates the system from its surroundings. The boundary of a system can be fixed or movable.

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20
Q

Closed system

A

consists of a fixed amount of mass (control mass), and no mass can cross its boundary. But energy, in the form of heat or work, can cross the boundary.

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21
Q

Isolated system

A

is a closed system in which energy is not allowed to cross the boundary.

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22
Q

Open system

A

is any arbitrary region in space through which mass and energy can pass across the boundary.

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23
Q

Control volume

A

(also see open system) is any arbitrary region in space through which mass and energy can pass across the boundary. Most control volumes have fixed boundaries and thus do not involve any moving boundaries. A control volume may also involve heat and work interactions just as a closed system, in addition to mass interaction.

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24
Q

Property

A

is any characteristic of a system. Some familiar properties are pressure P, temperature T, volume V, and mass m. The list can be extended to include less familiar ones such as viscosity, thermal conductivity, modulus of elasticity, thermal expansion coefficient, electric resistivity, and even velocity and elevation.

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25
Q

Extensive properties

A

are those whose values depend on the size—or extent—of the system. Mass m, volume V, and total energy E are some examples of extensive properties. Extensive properties of a nonreacting ideal- or real-gas mixture are obtained by just adding the contributions of each component of the mixture.

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26
Q

ecific properties

A

are extensive properties per unit mass. Some examples of specific properties are specific volume (v = V/m) and specific total energy (e = E/m).

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27
Q

Continuum

A

is a view of mass as continuous, homogeneous matter with no holes. Matter is made up of atoms that are widely spaced in the gas phase. Yet it is very convenient to disregard the atomic nature of a substance. The continuum idealization allows us to treat properties as point functions, and to assume the properties to vary continually in space with no jump discontinuities. This idealization is valid as long as the size of the system we deal with is large relative to the space between the molecules. This is the case in practically all problems, except some specialized ones.

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28
Q

Rarefied gas flow theory

A

applies to a substance in which the mean free path of its molecules is large compared to the characteristic length of the systems such that the impact of individual molecules should be considered, and the substance cannot be modeled as a continuum.

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29
Q

Density

A

is mass per unit volume.

30
Q

Specific volume

A

is the reciprocal of density and is defined as the volume per unit mass.

31
Q

Specific gravity, or relative density

A

is the ratio of the density of a substance to the density of some standard substance at a specified temperature (usually water at 4°C, for which the density is 1000 kg/m3).

32
Q

Specific weight

A

is the weight of a unit volume of a substance and is determined from the product of the local acceleration of gravity and the substance density.

33
Q

State

A

is the condition of a system not undergoing any change gives a set of properties that completely describes the condition of that system. At this point, all the properties can be measured or calculated throughout the entire system.

34
Q

Equilibrium

A

implies a state of balance. In an equilibrium state there are no unbalanced potentials (or driving forces) within the system. A system in equilibrium experiences no changes when it is isolated from its surroundings.

35
Q

Thermal equilibrium

A

means that the temperature is the same throughout the entire system.

36
Q

Mechanical equilibrium

A

is related to pressure, and a system is in mechanical equilibrium if there is no change in pressure at any point of the system with time.

37
Q

Phase equilibrium

A

is the condition in which the two phases of a pure substance are in equilibrium when each phase has the same value of specific Gibbs function. Also, at the triple point (the state at which all three phases coexist in equilibrium), the specific Gibbs function of each one of the three phases is equal.

38
Q

Chemical equilibrium

A

is established in a system when its chemical composition does not change with time.

39
Q

State postulate

A

specifies the number of properties required to fix the state of a system: The state of a simple compressible system is completely specified by two independent, intensive properties.

40
Q

Simple compressible system

A

is a system in which there is the absence of electrical, magnetic, gravitational, motion, and surface tension effects. These effects are due to external force fields and are negligible for most engineering problems.

41
Q

Independent properties

A

exist when one property can be varied while another property is held constant.

42
Q

Path functions

A

are functions whose magnitudes depend on the path followed during a process as well as the end states.

43
Q

Quasi-static, or quasi-equilibrium, process

A

is a process which proceeds in such a manner that the system remains infinitesimally close to an equilibrium state at all times. A quasi-equilibrium process can be viewed as a sufficiently slow process that allows the system to adjust itself internally so that properties in one part of the system do not change any faster than those at other parts.

44
Q

Isothermal process

A

is a process in which the temperature is maintained constant.

45
Q

Isobaric process

A

is a process during which the pressure P remains constant.

46
Q

Isochoric process

A

(isometric process) is a process during which the specific volume v remains constant.

47
Q

steady

A

no change with time opposite is unsteady

48
Q

uniform

A

no change with location over a specified region

49
Q

Steady-flow process

A

is a process during which a fluid flows through a control volume steadily. That is, the fluid properties can change from point to point within the control volume, but at any point, they remain constant during the entire process. During a steady-flow process, no intensive or extensive properties within the control volume change with time.

50
Q

Thermal equilibrium

A

means that the temperature is the same throughout the entire system.

51
Q

Zeroth law of thermodynamics

A

states that if two bodies are in thermal equilibrium with a third body, they are also in thermal equilibrium with each other. By replacing the third body with a thermometer, the zeroth law can be restated as two bodies are in thermal equilibrium if both have the same temperature reading even if they are not in contact.

52
Q

Celsius scale

A

(formerly called the centigrade scale; in 1948 it was renamed after the Swedish astronomer A. Celsius, 1701–1744, who devised it) is the temperature scale used in the SI system. On the Celsius scale, the ice and steam points are assigned the values of 0 and 100°C, respectively.

53
Q

Fahrenheit scale

A

(named after the German instrument maker G. Fahrenheit, 1686–1736) is the temperature scale in the English system. On the Fahrenheit scale, the ice and steam points are assigned 32 and 212°F.

54
Q

Thermodynamic temperature scale

A

is a temperature scale that is independent of the properties of the substances that are used to measure temperature. This temperature scale is called the Kelvin scale, and the temperatures on this scale are called absolute temperatures. On the Kelvin scale, the temperature ratios depend on the ratios of heat transfer between a reversible heat engine and the reservoirs and are independent of the physical properties of any substance.

55
Q

Kelvin scale

A

is the thermodynamic temperature scale in the SI and is named after Lord Kelvin (1824–1907). The temperature unit on this scale is the kelvin, which is designated by K (not °K; the degree symbol was officially dropped from kelvin in 1967). The lowest temperature on the Kelvin scale is 0 K.

56
Q

Kelvin

A

is the temperature unit of the Kelvin scale in the SI.

57
Q

Rankine scale

A

named after William Rankine (1820–1872), is the thermodynamic temperature scale in the English system. The temperature unit on this scale is the rankine, which is designated by R.

58
Q

Rankine

A

is the temperature unit for the Rankine scale in the English system.

59
Q

Ideal-gas temperature scale

A

is a temperature scale that turns out to be identical to the Kelvin scale. The temperatures on this scale are measured using a constant-volume gas thermometer, which is basically a rigid vessel filled with a gas, usually hydrogen or helium, at low pressure. The temperature of a gas is proportional to its pressure at constant volume.

60
Q

Pressure

A

is defined as the force exerted by a fluid per unit area.

61
Q

Pascal

A

(Pa) is the unit of pressure defined as newtons per square meter (N/m2).

62
Q

Absolute pressure

A

is the actual pressure at a given position and it is measured relative to absolute vacuum (i.e., absolute zero pressure). Throughout this text, the pressure P will denote absolute pressure unless specified otherwise.

63
Q

Gage pressure

A

is the difference between the absolute pressure and the local atmospheric pressure.

64
Q

Vacuum pressure

A

is the pressure below atmospheric pressure and is measured by a vacuum gage that indicates the difference between the atmospheric pressure and the absolute pressure.

65
Q

Pascal’s law

A

allows us to “jump” from one fluid column to the next in manometers without worrying about pressure change as long as we don’t jump over a different fluid, and the fluid is at rest.

66
Q

Barometer

A

is a device that measures the atmospheric pressure; thus, the atmospheric pressure is often referred to as the barometric pressure.

67
Q

Manometer

A

is a device based on the principle that an elevation change of Δz of a fluid corresponds to a pressure change of ΔP/ρg, which suggests that a fluid column can be used to measure pressure differences. The manometer is commonly used to measure small and moderate pressure differences.

68
Q

Bourdon tube

A

named after the French inventor Eugene Bourdon, is a type of commonly used mechanical pressure measurement device which consists of a hollow metal tube bent like a hook whose end is closed and connected to a dial indicator needle.

69
Q

Pressure transducers

A

are made of semiconductor materials such as silicon and convert the pressure effect to an electrical effect such as a change in voltage, resistance, or capacitance. Pressure transducers are smaller and faster, and they are more sensitive, reliable, and precise than their mechanical counterparts.

70
Q

Piezoelectric transducers

A

also called solid-state pressure transducers, work on the principle that an electric potential is generated in a crystalline substance when it is subjected to mechanical pressure. This phenomenon, first discovered by brothers Pierre and Jacques Curie in 1880, is called the piezoelectric (or press-electric) effect. Piezoelectric pressure transducers have a much faster frequency response compared to the diaphragm units and are very suitable for high-pressure applications, but they are generally not as sensitive as the diaphragm-type transducers.

71
Q

Deadweight tester

A

is a mechanical pressure measuring device, which measures pressure directly through application of a weight.