61. What do you understand by internal energy of a gas?
According
to the first law of thermodynamics, the total amount of heat supplied to the
gas is utilized to increase its temperature and rest to do the work against the
external pressure. The increase in the temperature of a gas is due to it has to
do the work against the intermolecular force of attraction between gas
molecules to expand, when heated. Hence, the total energy required to increase
the temperature of a gas i.e. the energy required to do the work against the
intermolecular force of attraction between gas molecules is termed as the
internal energy of a gas.
62. Why has a gas two values of specific heat capacity?
When
the gas is compressed suddenly when no heat is supplied (i.e. dQ=0) from
outside then the temperature of the gas increases due to compression & its
specific heat is zero as
![](Heat4_files/image002.gif)
A
gas will have infinite specific heat if and only if the gas is heated in such a
way that its temperature is always constant (i.e. dt=0) but dQ is not equal to
zero. The specific heat capacity of a gas is given as:
![](Heat4_files/image004.gif)
As the specific
heat of the gas can have any value oscillating in between zero to infinity
depending on the matter in which the gas is being heated. But practically for
easy consideration, there are two specific heat of a gas & they are:
1.
Specific heat capacity at constant volume.
2.
Specific heat capacity at constant pressure.
63.
What happens to the internal energy of a gas during (a) isothermal expansion
(b) adiabatic expansion?
During
isothermal expansion, there is no change in the temperature so the internal
energy of the gas remains unaltered i.e. dU = 0.
During
adiabatic expansion, the work is done by gas at the expenses of its internal
energy. So, during adiabatic expansion the internal energy of a gas falls (dU =
-PdV).
64.
Show that the efficiency of a heat engine is always less than 100%.
The
efficiency of the heat energy is given by the relation:
![](Heat4_files/image006.gif)
where, T1 & T2 are
the temperature of the source and sink. For a heat engine to be perfectly
efficient, the factor
must be equal to zero. That means either T2 must
be zero or T1 must be infinite. Hence, it is impossible that the
temperature of the sink to be at absolute zero and also it is impossible that
the temperature of the source is infinite. Hence, the efficiency of the heat
engine is always less than 100%.
65.
"Heat cannot be converted completely into mechanical work". Is this
statement true? Explain.
"Heat
cannot be converted completely into mechanical work". This statement is
absolutely correct. The heat energy possessed by a body is the energy of the
random motions of the molecules. The kinetic energy of a moving body represents
the ordered motion which its molecules have superimposed on their random
motion. When we convert heat energy into work then we are trying to change the
random molecular motion into ordered motion. The thermal motions of molecules
are random, it is impossible to convert all random motions into an orderly
motion. So, heat cannot be converted completely into mechanical work.
66. Is the energy of a gas molecules zero at absolute zero of
temperature? Explain.
No, the energy of a gas molecules is not zero at
absolute zero of temperature. As the total energy of a gas is the sum of its
potential energy & kinetic energy. Here, the kinetic energy of gas directly
depends upon temperature but the potential energy is not. At higher
temperatures, there is a great dependency of potential energy with temperature,
but it is not the proportional one, as in case of kinetic. At absolute zero of
temperature, the kinetic energy of a gas is zero but some potential energy
still remains. So, the net energy of the gas is equal to the potential energy
of the gas. Hence, at absolute zero of temperature, the energy of a gas
molecules is not zero.
67. The oceans have tremendous amount of heat energy. Can't we
utilize that heat energy for doing mechanical work? Justify your answer.
As the heat engine must possess source (at higher
temperature) and sink (at lower temperature) in order to do the mechanical work
by the engine. In order to perform mechanical work in ocean, there must be flow
of heat from a source to sink according to the second law of thermodynamics. As
the oceans have tremendous amount of heat energy i.e. source but there is no
sink where the source can reject some heat energy to perform mechanical work.
As the sink is absent, no mechanical work is done. Hence, the heat energy can
not be utilized for doing mechanical work.
68. Why does the atmospheric air become cold when it rises up?
At higher altitudes of atmosphere, the air pressure
is less (The atmosphere can be considered to be a sea of air, where upper
atmosphere can be considered to be of less depth and lower atmosphere near the
surface of earth can be considered to deep down.). Then according to the
relation P = ρgh (h being the height of air available above it), the pressure
at higher altitudes would be less. Since temperature of a gas system depends on
the pressure, less pressure means less temperature. So when the atmospheric air
rises up, they are exposed to lesser pressure, the temperature would gradually
decrease.
69.
What is the reason for difference in temperature of air coming out of a balloon
due to its sudden bursting and the atmospheric air at the same place?
Yes,
a gas always works when it expands in volume. The work done W by the gas is
given by the relation: dW = PdV
where,
P is the pressure of the gas and dV is the change in volume.
70. Air pressure in cycle tyres increase during riding. Explain
why?
The
air pressure P inside the tyres is given by the relation:
where,
ρ is
the density of air molecules and cav
is the root mean square velocity of air molecules. Hence, the air pressure in
cycle tyres is directly proportional to the square of the root mean square
velocity of air molecules. As the air molecules inside the tyres are in
vigorous motion during riding, its root mean square velocity also increases.
Hence, the air pressure in cycle tyres increases during
riding.
71.
A half filled water bottle is shaken vigorously. Does its temperature change?
Explain
A
half filled water bottle if shaken vigorously then the mechanical energy
supplied is converted into heat energy (W = JQ) according to the conservation
of energy. So, the mechanical work done against the intermolecular force of
attraction between water molecules result in the increment of temperature of
water. As a result, the temperature of the water inside the bottle rises. So,
the there is change of temperature.
72.
The "efficiency of all engines are less than that of the Carnot
engine." Why?
As
the carnot engine is considered as an ideal engine (that cannot be realized in
practice) due to the fact that it is a reversible engine. In the carnot engine,
there should be no loss of heat & no friction. Hence, its efficiency is
always greater than other heat engines as there is loss of heat in other heat
engines i.e. heat rejected to the sink and some energy is being lost as heat
due to friction. Hence, an ideal concepts always dominates over practical
concepts. Hence, the efficiency of all engines are less than that of the carnot
engine.
73. "A carnot engine is called an ideal engine". Why?
A carnot engine is called an ideal engine because
it cannot be realized in practice as well as due to the fact that it is a
reversible engine. In the carnot engine, there should be no loss of energies.
All the process in a carnot engine is slow. Hence, a carnot engine is called an
ideal engine.
74. Refrigerator transfers heat from a cold body to a hot body.
Does this violate the second law of thermodynamics?
Second law of thermodynamics states that:
1.
No heat engine that works in a cycle completely converts heat energy into work.
2.
When a cold body and a hot body are brought in contact with one another then
heat always flows from the hot body to cold body. Or, It is impossible to
construct a heat engine where the heat flows from colder body to hotter body
without doing work in the working substance.
As
the refrigerator is a heat engine that extracts heat from a cold body and
transfers it to a hot body. This implies that a refrigerator is a heat engine
that works reverse as other heat engine does. But it doesn't violets the second
law of thermodynamics (which tell us that heat cannot by itself flow from a
colder body to a hotter body) as the refrigerator transfers heat from a colder
body to a hotter body by doing the work in the working substance. So, the
principle of refrigerator doesn't violet the second law of thermodynamics.
75.
Why will a refrigerator with a fixed amount of food consume more energy in a
warm room than in a cold room?
A
refrigerator is a heat engine that extracts heat from a cold body and transfers
it to a hot body by doing the work in the working substance. Higher the
difference in temperature between cold & hot body, more work is required to
be done by the refrigerator. In warm room, temperature difference is high but
in cold room, temperature difference is low. So, more work is to be done by the
refrigerator in a warm room than in a cold room. Hence, a refrigerator with a
fixed amount of food consume more energy in a warm room than in a cold room.
76. Why do diesel engines need no spark plugs?
In a
diesel engine, the air can be compressed adiabatically such
that its temperature reaches about 7000C
before mixing the diesel with air in the cylinder. This
temperature is quite enough for igniting the diesel. Hence,
Diesel engines need no spark plugs. Petrol, on the other
hand need higher temperature for combustion. So adiabatic
compression alone is not enough. Therefore a spark plug is used
in addition (in petrol engines) to raise that temperature
further at least for a moment and then start a chain reaction of
petrol with oxygen.
77. Under what condition, an expanding gas will have fall
in temperature?
In an
adiabatic process, neither heat is supplied to the system
nor extracted from the system but there is always change in
temperature of the system. In adiabatic expansion of a gas,
the work is done by the gas utilizing its internal energy.
Hence, the temperature of an expanding gas falls in
adiabatic expansion.