1 / 18

Refrigerators

Refrigerators. Physics 313 Professor Lee Carkner Lecture 13. Exercise #12 Engines. V 1 = 6.25X10 -4 m 3 , P 1 = 12X10 6 Pa, n = 3 moles P 1 V 1 g = P 2 V 2 g P 2 = P 1 V 1 g /V 2 g = 385 MPa h = 1 – T 1 /T 2 = 0.75 W = h Q H , Q H = nc V D T 23

Download Presentation

Refrigerators

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. Refrigerators Physics 313 Professor Lee Carkner Lecture 13

  2. Exercise #12 Engines • V1 = 6.25X10-4 m3, P1 = 12X106 Pa, n = 3 moles • P1V1g = P2V2g • P2 = P1V1g/V2g = 385 MPa • h = 1 – T1/T2 = 0.75 • W = hQH, QH = ncVDT23 • P3 = 500X106 Pa, V3 = 7.8X10-5 m3 • QH = (3)(3/2)(8.31)(1564-1205) = 13424 J

  3. Limits on Engines • Engines convert heat into work and waste heat • Second Law of Thermodynamics • An engine cannot have 100% efficiency

  4. 1st and 2nd Laws • Converting heat completely into work does not violate the 1st law • The second law is an independent statement

  5. Refrigerators • A refrigerator is a device that uses work to move heat from low to high temperature • A heat pump does this to heat a room (want large QH)

  6. How a Refrigerator Works • Fluid flows through the cold chamber and evaporates, adding heat QL to the fluid from the chamber • The fluid is pumped into the hot chamber and compressed, adding work W • The fluid condenses releasing heat QH

  7. Refrigerator Cycle Compressor (work =W) Gas QL QH Low Pressure High Pressure Heat removed from fridge by evaporation Heat added to room by condensation Liquid Expansion Valve

  8. Refrigerator Performance • The equivalent of efficiency for a refrigerator is the coefficient of performance K K = QL/(QH-QL) • Unlike efficiency, K can be greater than 1

  9. Air Conditioner • Air conditioners also have condensers that dry out the air

  10. Heat Pump • The heat removed from the inside of a refrigerator is ejected into the kitchen • A refrigerator that has the cold chamber as the outdoors and the hot chamber as the house is called a heat pump • Many heat pumps can be reversed in summer to function as air conditioners

  11. Refrigerators and the Second Law • You cannot move heat from low to high temperature without the addition of work

  12. Statements of the Second Law • Kelvin-Planck Statement: • Clausius Statement:

  13. Equivalence • One implies the other • For example: • A 100% efficient engine connected to a high T reservoir powering a refrigerator cooling a low T reservoir to the same high T reservoir • The refrigerator by itself is “legal” but the net effect to is move QL from low to high T with no other effect

  14. Engines and Refrigerators • Efficiency: h = W/QH = (QH-QL)/QH = 1 - (QL/QH) • Can rewrite using: • Coefficient of performance: K = QL/W = QL/(QH-QL) (refrigerator)

More Related