Intro to 2nd Law Flashcards

1
Q

Problems associated with First Law (These processes cannot occur even though they are not in violation of the first law.)

A
  1. A cup of hot coffee does not get hotter in a cooler room!!
  2. Transferring heat to a paddle wheel will not cause it to rotate!!
  3. Transferring heat to a wire will not generate electricity!!
How well did you know this?
1
Not at all
2
3
4
5
Perfectly
2
Q

MAJOR USES OF THE SECOND LAW

A
  1. The second law may be used to identify the direction of
    processes.
  2. The second law also asserts that energy has quality as well
    as quantity.
  3. The second law of thermodynamics is also used in
    determining the theoretical limits for the performance of
    commonly used engineering systems, such as heat engines
    and refrigerators, as well as predicting the degree of
    completion of chemical reactions.
How well did you know this?
1
Not at all
2
3
4
5
Perfectly
3
Q

Statements of THE SECOND LAW

A
  1. Kelvin-Planck Statement
    - it is impossible for any device that operates on a cycle to receive heat from a single reservoir and produce a net amount of work.
  2. Clausius Statement
    - it is impossible to construct a device that operates in a cycle and produces no effect other than the transfer of heat from a lower-temperature body to a higher-temperature body.
How well did you know this?
1
Not at all
2
3
4
5
Perfectly
4
Q

The devices that convert heat to work.

A
  1. They receive heat from a high-
    temperature source (solar energy, oil furnace, nuclear
    reactor, etc.).
  2. They convert part of this heat
    to work (usually in the form of a
    rotating shaft.)
  3. They reject the remaining waste heat to a low-temperature sink (the atmosphere, rivers, etc.).
  4. They operate on a cycle.
How well did you know this?
1
Not at all
2
3
4
5
Perfectly
5
Q

A hypothetical body with a relatively large thermal energy capacity (mass x specific heat) that can supply or absorb finite amounts of heat without
undergoing any change in temperature is called a

A

Thermal Energy Reservoir

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
6
Q

In practice, large bodies of water such as “blank” can be modeled accurately as
thermal energy reservoirs because of their large
thermal energy storage capabilities or thermal
masses.

A

oceans, lakes, and rivers as well as the atmospheric air

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
7
Q

A “blank” supplies energy in
the form of heat,

and a “blank” absorbs it.

A
  1. Source
  2. Sink
How well did you know this?
1
Not at all
2
3
4
5
Perfectly
8
Q

Review the Steam Power Plant Figure

A

May bayad picture huhu

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
9
Q

Why is it impossible to have 100 thermal efficiency?

A

The impossibility of having a 100% efficient heat engine is not due to friction or other dissipative effects. It is a limitation that applies to both the idealized and the actual heat engines.

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
10
Q

Statement in thermal efficiency

A
  • Even the most efficient
    heat engines reject almost
    one-half of the energy they
    receive as waste heat.
  • Some heat engines perform
    better than others (convert
    more of the heat they
    receive to work).
  • Every heat engine must waste some energy by transferring it to a low-temperature reservoir in order to complete the cycle, even under idealized conditions.
How well did you know this?
1
Not at all
2
3
4
5
Perfectly
11
Q

The transfer of heat from a low-
temperature medium to a high-
temperature one requires special devices called

A

refrigerators

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
12
Q

The working fluid used in the
refrigeration cycle is called a

A

refrigerant

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
13
Q

The most frequently used
refrigeration cycle is the

A

vapor-compression refrigeration cycle.

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
14
Q

The efficiency of a refrigerator is expressed in terms of the

A

coefficient of performance
(COP).

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
15
Q

Objective of refrigerator

A

to remove QL from the
cooled space.

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
16
Q

Objective of heat pump

A

to supply heat QH into the warmer space.

17
Q

Any device that violates the first or the second law.

A

Perpetual-motion machine:

18
Q

A device that violates the first law (by creating energy) is called a

A

PMM1

19
Q

A device that violates the second law is called a

A

PMM2

20
Q

Reversible process:

A

A process that can be
reversed without leaving any trace on the universe.

21
Q

A process that is not reversible:

A

Irreversible

22
Q

The factors that cause a process to be irreversible are called

A

irreversibilities

23
Q

Factors / conditions of irreversibilities.

A
  1. The conditions for mechanical, thermal, or chemical equilibrium, namely, thermodynamic equilibrium, are not satisfied.
  2. Dissipative effects, such as friction, viscosity, inelasticity,
    electric resistance, and magnetic hysteresis, are present.
24
Q

For a process to be reversible….

A
  1. It should be performed QUASI-STATICally.
  2. It should not be accompanied by Dissipative effects.
25
Q

Though the reversible processes perform the best, but they are concepts only, then why are we interested in reversible processes?

A

(1) they are easy to analyze and
(2) they serve as idealized models (theoretical limits) to
which actual processes can be compared.

26
Q

REVERSIBLE HEAT ENGINE CYCLE – for steady flow system

A

Reversible Isothermal Heat Addition (process 1-2, TH = constant)
Reversible Adiabatic Expansion (process 2-3, temperature drops from TH to TL)
Reversible Isothermal Heat Rejection (process 3-4, TL = constant)
Reversible Adiabatic Compression (process 4-1, temperature rises from TL to TH)

27
Q

REVERSIBLE HEAT ENGINE CYCLE – for stationary system

A

Reversible Isothermal Expansion (process 1-2, TH = constant)
Reversible Adiabatic Expansion (process 2-3, temperature drops from TH to TL)
Reversible Isothermal Compression (process 3-4, TL = constant)
Reversible Adiabatic Compression (process 4-1, temperature rises from TL to TH)

28
Q

THE CARNOT PRINCIPLE

A

The efficiency of an irreversible heat engine is always less than the efficiency of a reversible one
operating between the same two reservoirs.

29
Q

CARNOT PRINCIPLE – the corollary

A

The efficiencies of
all reversible heat
engines operating
between the same
two reservoirs are
the same.

30
Q

THE CARNOT HEAT ENGINE

A

Nth{ < Nth,rev: irreversible
= Nth,rev: reversible
> Nth,rev: impossible

31
Q

THE CARNOT REFRIGERATOR & HEAT PUMP

A

COPr{ < COPr,rev: irreversible
= COPr,rev: reversible
> COPr,rev: impossible

32
Q

Review the heat engine: source converted to work, the rest is rejected to sink

A

Bawal picture huhu