refrigeration thermodynamics professor lee carkner lecture 21

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Refrigeration Thermodynamics Professor Lee Carkner Lecture 21

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Page 1: Refrigeration Thermodynamics Professor Lee Carkner Lecture 21

Refrigeration

Thermodynamics

Professor Lee Carkner

Lecture 21

Page 2: Refrigeration Thermodynamics Professor Lee Carkner Lecture 21

Refrigeration

Generally involve 4 processes

There is an input of heat and work and an output of heat

Wnet,in + QL = QH

We can write the coefficient of performance as:

COPR = QL / Wnet,in = QL/(QH-QL)

Page 3: Refrigeration Thermodynamics Professor Lee Carkner Lecture 21

Carnot Refrigeration Cycle

Two isothermal and two isentropic processes

But serves as an upper limit on the

efficiency of any refrigerator operating between two temperatures

COPR,Carnot = 1 / (TH/TL -1)

Page 4: Refrigeration Thermodynamics Professor Lee Carkner Lecture 21

Ideal Refrigeration Cycle

The ideal refrigeration cycle consists of four processes: Isobaric heat rejection in a condenser Isobaric heat absorption in a evaporator

Similar to a reversed Rankine cycle

Less efficient but much cheaper and simpler

Page 5: Refrigeration Thermodynamics Professor Lee Carkner Lecture 21

Ideal Refrigerator Diagram

Page 6: Refrigeration Thermodynamics Professor Lee Carkner Lecture 21

Household Refrigerator

Page 7: Refrigeration Thermodynamics Professor Lee Carkner Lecture 21

COP of Refrigeration Cycle

The heat or work for each process is just h

The heats are: qH = (h2-h3)

The COP can be written: COPR = qL/win = (h1-h4)/(h2-h1)

Page 8: Refrigeration Thermodynamics Professor Lee Carkner Lecture 21

Solving Refrigerator Problems For the four key points in the cycle,

there are only two pressures

At point 1 (before compressor) the fluid is a saturated vapor and h1 = hg and s1 = sg at P1

At point 3 (before throttle) the fluid is a saturated liquid and h3 = hf at P3

Find all h’s to get qL, qH, w and COP

Page 9: Refrigeration Thermodynamics Professor Lee Carkner Lecture 21

Actual Refrigerator Cycles

The fluid may leave the evaporator superheated instead of saturated

The fluid may be subcooled (a compressed rather than a saturated liquid) when it exits the condenser

Can also define the isentropic efficiency of the

compressor

C = (h2s-h1)/(h2a-h1)

Page 10: Refrigeration Thermodynamics Professor Lee Carkner Lecture 21

Actual Refrigerator Diagram

Page 11: Refrigeration Thermodynamics Professor Lee Carkner Lecture 21

Refrigerants

Want a fluid with a low boiling point

Many of these fluids are toxic

First safe refrigerants were developed in the 1920’s

Unfortunately, CFCs destroy ozone which blocks out solar UV Newer, CFC-free refrigerants (like 134a) have

become very common since the 1980’s

Page 12: Refrigeration Thermodynamics Professor Lee Carkner Lecture 21

Refrigerant Properties

Need 5-10 deg temperature difference between refrigerant and hot or cold chamber for good heat transfer

To avoid air leaks

For the condenser you need to keep a temperature

above room temperature

Page 13: Refrigeration Thermodynamics Professor Lee Carkner Lecture 21

Next Time

Read: 11.6-11.9 Homework: Ch 11, P: 18, 31, 42, 55