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Home > History and Archaeology > History > Practical Laws and Data on the Condensation of Steam in Covered and Bare Pipes; To Which Is Added a Translation of Peclet's "Theory and Experiments on the Transmission of Heat Through Insulating Materials."
Practical Laws and Data on the Condensation of Steam in Covered and Bare Pipes; To Which Is Added a Translation of Peclet's "Theory and Experiments on the Transmission of Heat Through Insulating Materials."

Practical Laws and Data on the Condensation of Steam in Covered and Bare Pipes; To Which Is Added a Translation of Peclet's "Theory and Experiments on the Transmission of Heat Through Insulating Materials."


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This historic book may have numerous typos and missing text. Purchasers can download a free scanned copy of the original book (without typos) from the publisher. Not indexed. Not illustrated. 1904 Excerpt: ...and the cooling of the outer take place according to the same laws. Thus in designating by M the quantity of heat transmitted per square foot per hour we would have three expressions for M, one in terms of of the conductivity C of the material of the wall, the two others in terms of the coefficients K and K' of cooling by radiation and contact of air, from which equations we may deduce the values of t and t' in terms of known quantities. But if we employ Dulong's formulas for cooling (794-797 )the calculation would be impossible, and even admitting the simpler formulas of 789 and 790 we would be led to an equation of the second degree, rather complicated and extremely difficult to handle. It is better to admit for the cooling and the heating Newton's law (791) which is sufficiently exact for small differences of temperature, and besides in all calculations relative to the transmission of heat one can never expect more than a rather rough approximation because there are circumstances which are impossible to take into account, such as the increase of temperature of the outer surface according to its height above the ground, the action of the wind, of the sun, and so forth. According to this we have: M=C.(t- 2 M= Q (T..t) M= Q (t'.ej equations which give, T(C+Qe)+C0 efC+QeJ+TC 2C+Qe 2C+Qe M=CZ P-(a) 865. From this formula follow several important consequences. If Qe was very small relatively to 2C and could be neglected, the formula reduces to M=--(T-d) and the value of M would be independent of C and e, that is to say of the material of the body and of its thickness. This case may occur when the value of e is very small relatively to that of C. Consider for example lead, the poorest conductor among the metals, and for which C= 113; supposing the sur...


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Product Details
  • ISBN-13: 9781231184424
  • Publisher: Rarebooksclub.com
  • Publisher Imprint: Rarebooksclub.com
  • Height: 246 mm
  • No of Pages: 40
  • Spine Width: 2 mm
  • Width: 189 mm
  • ISBN-10: 1231184426
  • Publisher Date: 01 May 2012
  • Binding: Paperback
  • Language: English
  • Returnable: N
  • Weight: 91 gr


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Practical Laws and Data on the Condensation of Steam in Covered and Bare Pipes; To Which Is Added a Translation of Peclet's "Theory and Experiments on the Transmission of Heat Through Insulating Materials."
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