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Heat Pump

저작시기 2016.05 |등록일 2017.04.17 한글파일한컴오피스 (hwp) | 11페이지 | 가격 2,000원

목차

Ⅰ. Introduction
1. Objective for the Experiment
2. Basic Theory

Ⅱ. Method
1. Components
2. Procedure

Ⅲ. Result
1. Data Reduction 1
2. Data Reduction 2

Ⅳ. Discussion &Conclusion

본문내용

Introduction
1. Objective for the Experiment
To understand the HVAC system and vapor compression cycle system through the experimental accomplishment

2. Basic Theory [1]
1) Reversed Carnot Cycle
In studying the performance of refrigeration cycles the concept of the thermodynamically reversible cycle is useful. Two important characteristics of a reversible cycle are as follows:

- No refrigeration cycle can have a higher coefficient of performance than that of a reversible cycle operating between the same source and sink temperatures.

- All reversible refrigeration cycles operates between the same source and sink temperatures have identical coefficients of performance.

After satisfy these precondition, we can use carnot cycle.

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2. Procedure [3]
1) For the test, at first, the atmospheric pressure, the dry and wet bulb temperatures are measured.

2) Enter up the fan power of the Low, Medium and High while only main power is turned on. This is to calculate the power of the compressor.

참고 자료

Laboratory on Thermal/Fluid Engineering, Experiments on the Heat Pump System, 성균관대학교
Claus Borgnakke, Richard E. Sonntag, "THERMODYNAMICS 7th Edition", WILEY,
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