–Engineering Thermodynamics–
Ø Pressure,
temperature and volume control the physical porperties of a perfect gas.
Ø Boyle’s
law, Charles’ law and Gay-Lussac lawas are applicable for the behaviour of a
perfect gas.
Ø The
unit of temperature in S.I. unit is Kelvin.
Ø The
unit of time in S.I. unit is second.
Ø The
unit of length in S.I. unit is meter.
Ø The
unit of energy in S.I. unit is Joule.
Ø According
to Gay-Lussac law for a pefect gas, the absolute pressure fo given mass varies
directly as absolute temperature, is volume is kept constant.
Ø An
dieal gas as compared to the real gas at very high pressure occupies more
volume.
Ø General
gas equation- PV = mRT
Ø Gas
law are applicable for gases alone and not to vapours.
Ø According
to Dalton’s law, the total pressure of the mixture of gases is equal to sumof
the partial pressure of all.
Ø Oxygen,
Nitogen, Hydrogen can be regarded as gas so that gas laws could be applicable,
within the commonly encountered temperature limits.
Ø The
unit of pressure in the S.I. unit is Pascal.
Ø One
property at one of the states, provided all other properties are known.
Ø A
closed system is one in which mass does not cross boundaries of the system,
through energy may do so.
Ø Temperature
of gas is produced due to kinetic energy of molecules.
Ø According
to kinetic theory of gases, the absolute zero temperature is attained when
kinetic energy of the molecules is zero.
Ø Kinetic
theory of gases assumes that the collisions between the molecules are perfectly
elastic.
Ø The
pressure of a gas in terms of its mean kinetic energy per uint volume E is
equal to 2E/3.
Ø Superheated
vapour behaves approximately as a gas.
Ø Absolute
zero pressure will occur whn molecular momentum of the system becomes zero.
Ø No
liquid can exist as liquid at zero temperature.
Ø The
unit of power in S.I. unit is Watt.
Ø The
condition of perfect gas vaccum i.e. absolute zero pressure can be attained at
a temperatue of -273.16 degree calcius.
Ø Specific
heat of air at constant pressure is equal to 0.24
Ø Intensive
property of a system is one whose value does not depend on the mass of the
system, like temperature and pressure etc.
Ø Characterstics
gas ocnstant of a gas is equal to Cp-Cv=R
Ø The
behaviour of gases can be fully determined by 3 laws.
Ø The
ratio of two specific heats of air is equal to 1.41
Ø Boyle’s
law i.e. PV=Constant is applicable to gases only small range of pressure.
Ø Joule’s
law states that the internal energy of a gas is a function of temperature.
Ø The
same volume of all gases would represent their molecular weight.
Ø Regnault’s
law states that the specific heat of a gas remains constant at all temperatures
and pressures.
Ø An
open system is one in which both energy and mass cross the boundaries of the
system.
Ø According
to the Charles’ law all perfect gases change in volume by 1/273th of their
origional volume at 0 degree celcius chenge in temperatue when pressure remains
constant.
Ø Gases
have two values of specific heat.
Ø Accrding
to Avogadro’s hypothesis the molecular weights of all the perfect gases occupy
the same volume under conditiions of pressure and temperature.
Ø Extensive
property of a system is one which depends on the mass of system.
Ø Work
done in a free expansion process is zero.
Ø The
statement that molecular weights of all gases occupy the same volume is known
as Avogadro’s hypothesis.
Ø To
convert volumetric analysis to gravimetric analysis, the relative volume of
each constituent of the flue is multiplied by its molecular weights.
Ø If
a gas is heated against a pressure, keeping the volume constant, then work done
will be equal to zero.
Ø An
isolated system is one in which neither mass or energy crosses the boundaries
of the system.
Ø Properties
of substance like pressure, temperature and density, in thermodynamics
coordinates are point function.
Ø Heat
is not a property of the system.
Ø According
to Avogadro’s law for a given pressure and temperature, each molecule of gas
occupies some volume.
Ø Mixture
of ice and water from a heterogeneous system.
Ø Pressure,
temperature, volume, density, internal energy, enthalpy and energy are the
property of a system.
Ø On
weight basis, air contains 23 parts of Oxygen.
Ø Heat
is not the intensive property.
Ø Thermal
conductivity is not a path function.
Ø Work
done in an adiabatic process between a given pair of end state depends on the
end states only.
Ø Heat
and work are path function.
Ø Volume
is constant for a mole for most of the gases at a given temperature and
pressure.
Ø A
reversible polytropic process can be described by the equation PVn=C
Ø Some
heat transfer take place for reversible polytropic process.
Ø Specific
heat of air at constant volume is equal to 0.17
Ø Cp-Cv
= R/J
Ø The
value of polytripic exponent n is the reversible polytropic process usually
varies between 1.2 to 1.4
Ø If
the value of n is high in the polytropic process, then the compressor work
between given pressure limits will be less.
Ø The
value of n=1 in the polytropic process indicates it to be isothermal process.
Ø Solids
and liquids have one value of specific heat.
Ø The
index of compression n tends to reach ratio of specific heats when process is
isentropic and specific heat does not change with temperture.
Ø Change
in enthalpy of a system is the heat supplied at constant pressure.
Ø The
NTP stands for normal temperature and pressure.
Ø The
heat exchange process in which the product of pressure and volume remains
constant is known as hyperbolic process.
Ø The
internal energy of a system is a function of only absolute temperature.
Ø In
an isothermal process, the thermal energy of gas molecules ramins constant.
Ø Zeroth
law of thermodynamics states that if two systems are both in equilibrium with a
third system, they are in thermal equilibrium with each other.
Ø If
a certain amount of dry ice is mixed with same amount of water at 80 degree
celcius the final temperature of mixture will be zero degree celcius.
Ø The
bsis for mesuring thermodynamic property of temperature is given by zetoth law
of thermodynamics.
Ø One
watt is equal to 1 Nm/sec
Ø Work
done is zero for constant volume, for free expansion and throttling.
Ø For
dry steam gas laws can be used with minimum error.
Ø 1
Calorie = 0.427 Kgm
Ø On
volume basis air contains 21 parts of Oxygen.
Ø Universal
gas constant is defined as equal to product of the molecular weight of the gas
constant.
Ø The
value of the product of molecualr weight and the gas charactersitc constant for
all the gases in S.I. units is 83.14 J/K mol K
Ø The
molecular weight expressed in gm of all gases at NTP occupies a volume of
22.4Litres.
Ø All
engineering processes are irreversible.
Ø For
water, the internal energy and enthalpy are function of temprature only.
Ø In
a free expansion process work done is zero but hear increases.
Ø If
a gas vapour is allowed to expand through a very minute aperature then such a
process is known as throttling.
Ø The
specific heat of air increases with increase in temperature.
Ø If
a fluid expands suddenly into vaccum through an orifice of large diamension,
then such a process is called free expansion.
Ø Enthalpy
remains constant during throttling process.
Ø Isothermal and adiabatic processesa are
thrrmodynamically reversible.
Ø Throttling
is irreversible process.
Ø In
order that a cycle be reversible –
_ Free expansion or friction resisted expansion/compression process should not be encountered.
_ When heat is being absorbed, temperature of hot source and working substance should be same.
_ When heat is being rejected, temperature of cold source and working substrance should be same.
_ Free expansion or friction resisted expansion/compression process should not be encountered.
_ When heat is being absorbed, temperature of hot source and working substance should be same.
_ When heat is being rejected, temperature of cold source and working substrance should be same.
Ø For
a thermodynamic process to be reversible, the remperatue difference between hot
body and working substance should be zero.
Ø Minimum
work in compressor is possible when the value of adiabatic index n is equal to
1.
Ø The
more effective way of increasing efficiency of carnot engine is to decrease
lower temperature.
Ø Entropy
change depends on heat transfer.
Ø For
reversible adiabetic process, change in entropy is zero.
Ø Isochoric
process is one in which no mechanical work is done by the system.
Ø When
a gas flows through a very long pipe of uniform corss-section the flow is
approximately isothermal.
Ø The
work done is the expansion of a gas from volume V1 to V2 under constant
pressure P is equal to P(V2 - V1)
Ø An
expansion process as per law PV=Constant is known as hyberbolic process.
Ø Under
ideal conditions, isothermal, isobaric, isochoric and adiabatic processes are
quasi-static processes.
Ø During
throttling process enthalpy remains constant.
Ø When
liquid boils at constant pressure, the enthalpy increases.
Ø Maximum
work by an expansion of a gas in a closed system is possible when takes place
at constant pressure.
Ø Enthalpy
is the sum of internal energy, the pressure and volume product.
Ø Heat
energy stored in the gas and used for raising temperature of a gas is known as
intermal energy.
Ø Accoring
to first law of thermodynamics total energy of a system remains constant.
Ø Energy
can neither be created nor destroyed but can be converted from one form to
other if inferred from first law of thermodynamics.
Ø First
law of thermodynamics is furnishes the relationship between heat, work and
properties of system.
Ø Change
in enthalpy in a closed system is equal to heat transferred if the reversible
porcess takes place at constant volume.
Ø The
first law of thermodynamics was developed by Joule.
Ø According
to first law of thermodynamics heat and work are mutually convertible.
Ø Total
heat of a substance is also called as enthalpy.
Ø Addition
of heat at constant pressure to a gas results in raising its temperature and
doing external work.
Ø The
temperature in a process in which work is done by expanding a gas under
adiabatic condition will decrease.
Ø The
work given out duing expansion process in a closed system will increase when
the value of n decrease.
Ø The
work required for compression in a closed system increases when value of n
increases.
Ø Carnot
Cycle –
_It is represented as a standard of perfection.
_It provides concept of maximising work output between two temperature limits.
_The degree of perfection of other engine can be compared with carnot cycle.
_It has maximum efficiency for reversible cycle.
_It’s efficiency depends upon temperature range of operation.
_It is represented as a standard of perfection.
_It provides concept of maximising work output between two temperature limits.
_The degree of perfection of other engine can be compared with carnot cycle.
_It has maximum efficiency for reversible cycle.
_It’s efficiency depends upon temperature range of operation.
Ø Measurement
of operation of temperature is based on zeroth law of thermodynamics.
Ø Carnot
cycle efficiency is maximum when final temperature is 0 degree Kelvin.
Ø If
a heat engine attains 100% thermal efficiency, it violates second law of
thermodynamics.
Ø If
heat be exchanged in a reversible manner, entropy will change accordingly.
Ø If
a system after undergoing a series of processes, returns to the initial state
then sum of heat and work transfer will be zero.
Ø According
to Clausius Statement –
_ Heat flows from hot substance to cold substance unadided.
_ Heat can flow from cold substance to hot substnace with the aid of external work.
_ Heat flows from hot substance to cold substance unadided.
_ Heat can flow from cold substance to hot substnace with the aid of external work.
Ø A
Machine that continuously creates its own energy represents the perpetual
motion of the first kind.
Ø An
actual engine is to be designed having same efficiency as the carnot cycle.
Such a proposition is impossible.
Ø In
a carnot cycle, heat is transferred at constant temperature.
Ø Change
of entropy depends upon change of heat.
Ø The
value of Joule-Kelvin coefficient for an ideal gas is zero.
Ø The
value of entropy at 0 degree celsius is taken as zero.
Ø In
a cycle the heat is rejected at constant pressure.
Ø Steam
flow through a nozzle is considered as adiabatic process.
Ø Internal
energy of a substance depends on temperature.
Ø A
diathermic well is one which permits thermal interaction.
Ø An
adiabatic well is one which prevents thermal interaction.
Ø The
door of a running refrigerator inside a room was left open then the room will
be gradually warmed up.
Ø Compressed
air coming out from a punctured football becomes cooler.
Ø Water
contained in a beaker can be made to boil by passing steam through it at a
pressure greater than atmospheric pressure.
Ø Heat
can be converted into work.
Ø Heat
rays can ve converged at one point by concave mirror.
Ø Water
expands when cooled below 4 degree celcius.
Ø Heat
may transfer by any of three modes.
Ø During
throttling process heat exchange does not place, no work is done by expanding
steam and there is no change of internal energy of steam.
Ø The
energy of molecular motion appears as heat.
Ø A
sudden fall in the barometer reading is a sign of storm.
Ø Calorie
is a measure of quantity of heat.
Ø The
first law of thermodynamics is the law of conservation of energy.
Ø A
perpetual motion machine is a hypothetical machine whose operation would
violate tha laws of thermodynamics.
Ø Kelvin
Plank’s law deals with conversion of heat into work.
Ø According
to Clausis statement of second law of thermodynamics heat can’t be transferred
from low temperature to high temperature source without the aid of external
energy.
Ø A
frictionless heat engine can be 100% efficient only if its exhaust temperature
is 0 degree kelvin.
Ø Carnot
cycle consists of two isothermals and two isentropics.
Ø Tha
ratio of actual cycle efficienry to that of the ideal cycle efficiency is
called efficiency ratio.
Ø The
constant volume cycle is also called Otto cycle.
Ø Air
refrigerator work on Reversed Joule cycle.
Ø Rankine
cycle consists of five processes.
Ø Relative
efficiency of a gas power cycle is given as the ratio of actual thermal
efficiency to air standard efficiency.
Ø It
is proposed to make a direct heat-to-heat converter out of an elementary system
which absorbs heat while doing isothermal work exactly equal to the heat
absorbed, therby keeping internal energy constant. Such a system is not
possible.
Ø Maxwell’s
thermodynamic relation are applicable to chemical system in equilibrium.
Ø An
engine working between positive temperatures can not be a heat pump.
Ø A
refrigerator working between positive temperatues must take work out of work
reservoir.
Ø Thrmal
power plant works on Rankine cycle.
Ø Otto
cycle consists of two isentropisc and two constant columes processes.
Ø The
efficiency of a carnot cycle is depends on temperature of source and sink.
Ø For
same compression ratio and for same heat added Otto cycle is more efficient
than Diesel cycle.
Ø The
efficiency of Carnot cycle is maximum for reversible engine.
Ø For
the same compression ratio, the efficiency of dual combustion cycle is less
than otto cycle and greater than diesel cycle.
Ø Carnot
cycle is a reversible cycle.
Ø Diesel
cycle consists of two isentropics, one constant volume and one constant
pressure processes.
Ø If
both Stirling and Carnot cycles operates within the same temperature limits
then efficiency of Stirling cycle as compared to Carnot cycle is equal.
Ø Stirling
and Ericsson cycles are reversible cycle.
Ø The
working substance for acarnot cycle is ideal gas.
Ø A
cycle consisting of two adiabatics and two constant pressure processes is known
as Joule cycle.
Ø Reversed
joule cycle is called Brayton cycle.
Ø Brayton
cycle sonsists of two isentropics and two constant pressure processes.
Ø The
cycle in which heat is supplied at constnat volume and rejected at ocnstant
pressure is known as Atkinson cycle.
Ø The
efficiency of Diesel cycle with decrease in cut off increase.
Ø The
ideal efficiency of a Brayton cycle without regeneratio with increase in
pressure ratio will increase.
Ø The
ideal efficiency of a Brayton cycle with regeneration, with increase in
pressure ratio will decrease.
Ø Reversed-Brayton
cycle is used for air craft refrigeration.
Ø Gas
turbine cycle consists of two isentropics and two constant pressure processes.
Ø The
thermodynamic difference between a Rankine cycle working with saturated steam
and the Carnot cycle is that heat is supplied to water at temperature below the
maximum tempereture of the cycle.
Ø The
heat addition in dual combustion cycle is done at partly at constnat pressure
and partly at constant volume.
Ø Diesel
cycle efficiency is maximum when the cut off is zero.
Ø The
pressure ratio in case of Bell-coleman cycle is of the order of 10-15.
Ø Stirling
cycle consists of two isothermals and two constant volumes processes.
Ø Atkinson
gas engine has a special feature that isentropic compression is on a short
stroke and the expansion on longer stroke.
Ø The
ideal efficiency of an Ericsson cycle with perfect regenration and operating
between two given temperature limits is equal to carnot cycle.
Ø In
a Carnot engine, when the working substance rejects its heat to sink, the
temperature of sink remains same.
Ø The
ideal efficiency of Joule cycle operating between two given temperature limits
is less than carnot cycle.
Ø The
ideal efficiency of a Striling cycle with perfect regeneration and operating
between two given temperature perature limits is equal to Carnot cycle.
Ø The
concept of regeneration is used in Stirling and Ericsson cycles.
Ø A
Bell-coleman cycle is a reversed Joule cycle.
Ø Ericsson
cycle consists of two isothermals and two consrnat pressure processes.
Ø A
petrol engine theoretically operates on constant volume cycle.
Ø A
diesel engine theoretically opeartes on constant pressure cycle.
Ø A
high speed diesel engine theoretically operates on mixed cycle of constant
pressure and constant volume.
Ø A
constant pressure gas turvine works on the Brayton cycle.
Ø According
to Kelvin-Plank’s statement, it is impossibe to construct a heat engine which
operates in a cycle and receives a given amount operates in a cycle and
receives a given amount of heat from a high temperature body and does equal
amount of work.
Ø A
steam nozzle converts heat energy into kinetic energy.
Ø According
to Clausius statement it is impossible to construct a device which operates in
a cycle and produces no effect other than the reansfer of heat from cooler body
to hotter body.
Ø Under
condition that hot resevoir is at negatice temperature, it is possible that
heat be abstraced from hot source, as well as cold source and positive work be
done.
Ø According
to Pettlier Thomson effect when two dissimilar metals are heated at one end and
cooled at other, e.m.f. is developed proportional to dieefrence of temperature
at two ends.
Ø All
diesel cycles except slow speed engine use mixed dual.
Ø Second
law of thermodynamics defines entropy.
Ø Gas
turvine works on constant pressure cycle.
Ø Cycle
used in thermal power plant is Rankine.
Ø An
isentropic process on T-S diagram is represented by vertical line.
Ø Expansion
in nozzle is a adiabatic process.
Ø Air
standard efficiency of a diesel cycle is dependent upon ratio of specific
heats, cut off ratio and chemical equilibrium.
Ø Entropy
is called the property of the system because it has a single value at each
equilibrium state.
Ø When
two gases suddenly mix up with each other then resultant entropy of the system
will increase.
Ø If
hot water and cold water are mixed, then the entropy of the system will
increase.
Ø When
a process undergoes a complete cycle then the change of entropy will be zero.
Ø If
air is compressd adiabatically from atmospheric condition in a cylinder having
compression ratio of 6 then pressure at the end of the compression shall be greater
than 6 ata.
Ø A
process which undergoes enegy loss due to friction is called irreversible
process.
Ø Density
is not an extensive property.
Ø Internal
energy and enthalpy of an idle gas are funcitons of temperature only.
Ø A
process occurs spontaneously of its entropy increases.
Ø The
areas under the curve on T-S diagram represents the heat transfer for
reversible processes.
Ø Work
is considered to be superior from of energy as compated to heat energy because
while work can be fully converted into heat, heat can’t be fully converted into
work.
Ø Triple
point of a pure substance is a point of which solid, liquid and vapour phases
exit together.
Ø A
substance above critical temperature exists as supersaturated fluid.
Ø One
kilowatt hour of energy is equal to 3600KJ.
Ø All
the reversible engines working between the same temperature limits have same
efficiency.
Ø It
is not possible to liquefy hydrogen at room temperature by application of
pressure because its critical temperature is lower than room temperature.
Ø All
gases behave ideally under low pressure conditions.
Ø Otto cycle is more efficient than Diesel cycle for a given compression ratio.
Ø RMS
velocity of hydrogen gas at NTP is 1839 m/sec.
Ø Atom
is defined as the element made up of minute and chemecally indivisible
particles.
Ø Element
is defined as the substance which has not been resolved into simper from.
Ø Work
done during a process can be determined by integration of pdV when the process
is quasi-static.
Ø During
a process on the closed system, its internal energy increases by twice the
units than the heat aded to it. It is possible due to performing of shaft work
on the system.
Ø Partial
pressure of a component in a mixture is pressure of the component itself if it
was present in the entire volume at the same temperatue.
Ø Siblimation
curve on p-t diagram for all substances possesses the positive slope.
Ø The
process of sublimation is found to occur in the case of solid Carbondioxide.
Ø Vaporisation
curve on p-t diagram for all substance possesses positive slope.
Ø When
a vapour condenses into a liquid it evolves heat.
Ø Sometimes
ice is white in colour. It is due to presence of dissolved air/gases and
impurities.
Ø Bomb
calorimeter is used to measure the calorific value of solid or liquid fuel.
Ø Avogadro’s
hypothesis is concerned with the combustion of gaseous fuels.
Ø The
area under a curve on T-S diagram represents heat transfer during reversible
process.
Ø Submerged
combustion involves combustion inside the liquid medium.
Ø All
the commercial liquid fuels are derived from crude oil.
Ø Specific
fuel consumption is defined as fuel consumed per hour per BHP.
Ø Flameless
combustion means catalytic combustion.
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