| convert thermal energy into mechanical
energy |
|
| lead to a more ordered state |
|
| cannot be reversed |
|
| do not conserve energy |
| heat energy to flow from a colder body to
a hotter body |
|
| an ideal heat engine to have the
efficiency of 99% |
|
| an ideal heat engine to have non-zero
power. |
|
| a physical process to yield more energy than what is put in |
| The temperature outside equals the
temperature inside of the refrigerator. |
|
| The rate at which heat is removed from the
inside equals the rate at which heat is delivered
outside. |
|
| The power consumed by the refrigerator
equals the rate at which heat is removed from the
inside. |
|
| The power consumed by the refrigerator equals the rate at which heat is delivered to the outside. |
| the amount of heat consumed per
second |
|
| the temperature of the cold
reservoir |
|
| the temperature of the hot
reservoir |
|
| the size of the cold reservoir |
|
| the size of the hot reservoir |
| Increase the mechanical work
input. |
|
| Decrease the outside
temperature. |
|
| Decrease the inside
temperature. |
|
| Increase the outside temperature. |
| Because it is impossible for even a
perfect engine to convert heat entirely into mechanical
work. |
|
| Because the cold reservoir keeps the
engine from overheating. |
|
| Because the cold reservoir keeps the
engine from overcooling. |
|
| Because the cold reservoir increases the power of the engine. |
The concept required to solve the given problem is second law of thermodynamics.
Use the properties of second law of thermodynamics and then find out the correct option.
Second law of thermodynamics: It states that total entropy can remain uniform in ideal cases where the system is in a steady state.
(A)
A thermodynamic process is one which converts the heat energy into the mechanical energy and some of the heat into the surroundings.
During the conversion of heat energy into the mechanical energy, the total heat energy cannot be converted. Some energy will always be lost to the surrounding. During the thermodynamic process, total energy is conserved.
The thermodynamic process that occurs in nature is irreversible process and cannot be reversed back.
(B)
According to the properties of second law of thermodynamics, it is possible to transfer the heat from colder body to the hotter body without the help of any external agency. No ideal heat engine exists with efficiency about 100%. From the law of conservation of energy, it is impossible to get more output than input under any physical process.
(C)
The coefficient of performance of a refrigerator is,

Here, QC is the quantity of heat removed from the cold reservoir and W is the work done.
Substitute
for W in above equation.

Here, TC is the temperature of cold body and TH is the temperature of cold body and QH is the heat supplied to the hot reservoir.
Substitute 1 for COP, then

It implies that the heat removed from the inside is equal to the power consumed by the refrigerator.
(D)
The efficiency of a heat engine is,

From the equation, to increase the efficiency of a heat engine, either the temperature of the cold reservoir will be decrease or the temperature of the hot reservoir will be increase.
(E)
The coefficient of performance of a refrigerator is,

Here, QC is the quantity of heat removed from the cold reservoir and W is the work done.
Substitute
for W in above equation.

Here, TC is the temperature of cold body and TH is the temperature of cold body and QH is the heat supplied to the hot reservoir.
To increase the value of COP, the value of TH will be decrease.
(F)
Heat engine can never convert total heat energy into mechanical energy. So therefore, the heat engine must have a cold reservoir because it is impossible for even a perfect engine to convert heat entirely into mechanical work.
Ans: Part AThe thermodynamic process that occurs in nature cannot be reversed.
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