Power Plant Engineering - Thermodynamics and Cycles Review

0.0(0)
Studied by 0 people
call kaiCall Kai
Locked
learnLearn
examPractice Test
spaced repetitionSpaced Repetition
heart puzzleMatch
flashcardsFlashcards
GameKnowt Play
Card Sorting

1/45

flashcard set

Earn XP

Description and Tags

Vocabulary flashcards covering core concepts, properties, laws, and gas/steam power cycles from Power Plant Engineering Days 1 through 4.

Last updated 2:24 PM on 9/11/26
Name
Mastery
Learn
Test
Matching
Spaced
Call with Kai
Chat

No analytics yet

Send a link to your students to track their progress

46 Terms

1
New cards

Thermodynamics

The study of heat and work.

2
New cards

Pure substance

A working substance whose chemical composition remains the same even if there is a change in phase (e.g., water).

3
New cards

Ideal gas

A working substance which remains in a gaseous state during its operating cycle and whose equation of state is PV=mRTPV = mRT (e.g., air).

4
New cards

Pressure

In general, the ratio of force per unit area.

5
New cards

Gage pressure

The pressure reading from the gage pressure instrument which is higher or lower than the atmospheric pressure.

6
New cards

Vacuum pressure

A pressure reading that is less than atmospheric pressure.

7
New cards
<p>Absolute pressure</p>

Absolute pressure

The pressure measured relative to absolute zero pressure, equal to the sum of gauge pressure and atmospheric pressure: Pabs=Pg+PatmP_{abs} = P_g + P_{atm}.

8
New cards

Temperature

The degree of hotness or coldness of a substance or body.

9
New cards

Pyrometer

An instrument used to measure high temperature gases.

10
New cards

Density

In thermodynamic terms, the mass per unit volume of a substance (w=mVw = \frac{m}{V}).

11
New cards

Specific volume

The volume per unit mass of a substance (v=Vmv = \frac{V}{m}), which is also the reciprocal of density.

12
New cards

Specific gravity

The ratio of the density of a substance to the density of a standard fluid (water for liquid and air for gas).

13
New cards

Internal Energy (UU)

The heat energy due to the movement of molecules within a substance brought about by its temperature.

14
New cards

Flow Work

The energy necessary to push a mass into or out of a control volume, given by pressure times specific volume (Wf=PvW_f = P v).

15
New cards

Enthalpy (HH)

The total heat content of a system, equal to the sum of internal energy and flow work (h=U+Pvh = U + P v).

16
New cards

Stagnation Enthalpy

Enthalpy given by the equation hs=ho+vo22000h_s = h_o + \frac{v_o^2}{2000}, where vov_o is initial velocity and hoh_o is ordinary enthalpy.

17
New cards

Entropy (SS)

A measure of unavailable energy or molecular randomness, calculated as heat transferred divided by temperature (S=QTS = \frac{Q}{T}).

18
New cards

Potential Energy (PP)

An energy produced due to a change in elevation (P=mghP = mgh).

19
New cards

Kinetic Energy (KEKE)

An energy produced due to the mass and velocity of a body (KE=12mv2KE = \frac{1}{2} m v^2).

20
New cards

Work (WW)

The product of the displacement of a body and the component of force in the direction of displacement (Work=Force×Distance\text{Work} = \text{Force} \times \text{Distance}).

21
New cards

Zeroth Law of Thermodynamics

States that when two bodies are in thermal equilibrium with a third body, they are in thermal equilibrium with each other and hence are at the same temperature.

22
New cards

First Law of Thermodynamics

States that one form of energy may be converted into another form, meaning all energy entering a system equals all energy leaving.

23
New cards

Second Law of Thermodynamics (Kelvin-Planck Statement)

States that it is impossible to construct a heat engine which operates in a cycle and receives a given amount of heat from a high temperature body and does an equal amount of work.

24
New cards

Third Law of Thermodynamics

States that the absolute entropy of a pure crystalline substance in complete internal equilibrium is zero at zero degrees absolute.

25
New cards

Boyle's Law

Ideal gas law stating that at constant temperature, pressure and volume are inversely proportional (P1V1=P2V2P_1 V_1 = P_2 V_2).

26
New cards

Charles's Law

Ideal gas law stating that at constant pressure or constant volume, temperature varies directly with pressure or volume (T1P1=T2P2\frac{T_1}{P_1} = \frac{T_2}{P_2} and V1T1=V2T2\frac{V_1}{T_1} = \frac{V_2}{T_2}).

27
New cards

Reversible Process

An ideal thermodynamic process occurring with no friction loss.

28
New cards

Adiabatic Process

A process in which there is no heat gain and no heat loss (Q=0Q = 0), as the system is perfectly insulated.

29
New cards

Constant Volume Process

A thermodynamic process occurring at constant volume (V1=V2V_1 = V_2); also called isometric, isochoric, or isovolumic process.

30
New cards

Constant Pressure Process

A thermodynamic process occurring at constant pressure (P1=P2P_1 = P_2); also called an isobaric process.

31
New cards

Constant Temperature Process

A thermodynamic process occurring at constant temperature (T1=T2T_1 = T_2); also called an isothermal or hyperbolic process.

32
New cards

Isentropic Process

A reversible adiabatic process where entropy remains constant (Δs=0\Delta s = 0) and governing equation is PVk=cP V^k = c.

33
New cards

Polytropic Process

An internally reversible process governed by the relationship PVn=cP V^n = c, where nn is the polytropic index.

34
New cards

Carnot Cycle

The most efficient thermodynamic cycle, consisting of two constant temperature (isothermal) processes and two isentropic processes.

35
New cards

Otto Cycle

A thermodynamic power cycle modeling a spark-ignition type engine, featuring constant volume heat addition and rejection.

36
New cards
<p>Diesel Cycle</p>

Diesel Cycle

A thermodynamic power cycle modeling a compression-ignition type engine, featuring constant pressure heat addition and constant volume heat rejection.

37
New cards

Brayton Cycle

An open cycle gas turbine system consisting of an isentropic compressor, constant pressure combustor, isentropic turbine, and generator.

38
New cards

Sub-cooled liquid

A liquid at a temperature lower than its saturation temperature for a given pressure, so it is not about to vaporize; also known as compressed liquid.

39
New cards

Saturated liquid

A liquid that exists at its boiling temperature and is about to vaporize with any addition of heat.

40
New cards

Saturated vapor

A vapor at its condensation temperature that is about to condense with any removal of heat.

41
New cards

Superheated vapor

A vapor at a temperature higher than its saturation temperature for a given pressure, so it is not about to condense.

42
New cards

Critical point

The state point on a phase diagram at which the properties of saturated liquid and saturated vapor become identical.

43
New cards
<p>T-s Diagram regions for Pure Substance</p>

T-s Diagram regions for Pure Substance

Diagram illustrating the subcooled region, wet/mixture region, superheated region, saturated liquid line, saturated vapor line, and critical point.

44
New cards

Quality (xx)

The ratio of the mass of vapor to the total mass of liquid and vapor mixture (x=mvmL+mvx = \frac{m_v}{m_L + m_v}).

45
New cards

Moisture (yy)

The ratio of the mass of liquid to the total mass of vapor and liquid mixture (y=1x=mLmL+mvy = 1 - x = \frac{m_L}{m_L + m_v}).

46
New cards
<p>Rankine Cycle</p>

Rankine Cycle

The most common steam power cycle consisting of a boiler, turbine, condenser, and pump, using water as its working fluid.