(PDF) 95/02109 Computation of temperatures and stresses of fluid-conducting pipes on the basis of the temperature variation on the outer surface - DOKUMEN.TIPS (2024)

16 Fuel science and technology (tindsmentsl science, analysis, instrumentation)

g5/020% Uss of alkalino fly aah as an ??mondmant for awlns manun Vincini, M. et aL, BiorcFourcc Technolo~, 1994, 49, Alkaline fly ash was characterized for the leaching potenti and minor constituents. and then added to swine maure at 10% and 2 w/v ratio. The irdluen& of fly ash on microbial production of CO, was studid during a 12day ex+mental period. pH, ammonium- and total N, organic C, available 8, avadable and more refracto fractions of P, K, Mg, Cu, Fe, Mn and Zn were determined on the fly as x -amended manwe. On the basis of the results, it a

BP” ars

which occwrcd in the amen that the reduction in CO, production

ed manure was probably due to the_ hi@ pH values of the manure caused by fly ash addition, rather than to an mlubihon of microbial activity and respuatlon.

%mo% Vltriffcatlon of rsslduss Warmer Bulletin, Feb. 1995, (441, p. 24.

Short note on a recent US blicatlon dealing with combustion residues by the ASMENS Bureau of &es.

95/02100 Working for a ckaner burn Morris, T. A and Vecci, S. J. MPS, Modern Power Systems, Dec. 1994, 14, (12), 33-35. Reports that Babco*ck Bt Wilcox has constructed a state-of-the-art tes!facil- ity that will integrate combustion and post-combustion testin capabtibes. An important role of this facility is that it will enhance B&W s capabilities to provide the products and processes that are needed to meet the require- ments of the USA Clean Air Act Amendments of 1990 and future regula- tions on air toxics.

%I021 01 World dlnctory of snvlronmsntal organlsationa Earthscan Publications, 120 Pentonville Rooci, London Nl OJA? f40.00.

16 FUEL SCIENCE AND TECHNOLOGY

Fundamental Science, Analysis, Instrumentation

95/02102 Ana sir of gallium In rock-coal by XRF L$, hf. 1 Huancc S & 1993,34, (7,328-330, (In Fese) DIED a study of the determmauon of gallmm 111 coal by an XRF

%/02102 Appllcatlon of a UV-curlng rssln to hydrodynamic atudiss In porous msdla $ZZ~anlS. E. et al., Id. Eng. Chem. Res., Aug. 1994, 33, (8),

Laboratoi techniques which have been applied to visualization of flow and transport in porous media include light transmission, matched index of refraction methods, NMR techniques, and use of epoxies. Within the pre- sent studv. a commercisllv available UV-curinn resin is anulied to caohu- ing trans~rt behaviour in’ porous media. This-technique * ’ ovides seieral capabiliues including rapid solidification of soil stmcture/ ff- md distribution at preselected locations without stopping flow and the ability to cure the structure of fluid interfaces. This resin holds promise to enhance the ability to study flow and transport through porous media, including the study of oarticle transnort. hvdrodvnamic disoersion. fluid distribution in multi- ihase flow, ahd &$&g-during b&ration.

%I02104 BMS hsl s BT to mob the right connactlons Enerp ln Buildings & ndustry, Nov.-Dec. 1994,13, (lo)! p. 70. P

Describes how a Slebe building management system is helpmg ensure that BT’s Madley Communications Centre in Herefordshire operates smoothly 24 hours a day, 365 days a year.

%I021 05 CARS tempsraturs msasursmenta In s Sasol- and msthanol-furllsd internal combustion englns Ball, D. et al., S. Afr. J. Sci, 1994, 90, (6), 343-347. The temperature inside the cylinder pf a MeOH-fue1e.d and Sel-fueled

measured by coherent anu- tokes Raman spectrosco single-cylinder msearcb tnp runmng under lmock$gs$o~;&‘a

sure was measured with a piexoelectric transducer. duced by Fischer-Tr alcohol-rich camp aXch

e Sasol fuelt+ pro- and related refining processes, are olefimc and

with conventional petroleum fuels. The results can be used for eneralized chemical modelling of engine knock, or two-zone modelling o f * m-cylinder combustion.

%I02106 Charactarlzatlon of gol&,nucksr aromatk sulfur hstrrocycles In a co+ sxtract by C 8 ‘v%+&~,$. et al., Ranbao Huanre Xuebao, 1994, 22, (2), 196-202. (In

Bslo2107 Charactrrlutlon of tha flow transition bstwssn bubbling and turbulent fluidlzation Ch3~lx;g~ A. er al., Ind. Eng. Chem. Res., Aug. 1994, 33, (8),

A lot of coitmversy exists in the literature on the actual boundaries of the turbulent regime in gas-solid fluidixation. The work in this that this disagreement results from the

per shows q ta?techniques

used. It is found that the onset of turbulent e of experimen uidization is at lJ$ and that the

velocity U, which has often been reported in the literature, I an ardfact due to the use of differential pressure transducers. to settle the dispute.

The aim of the paper is

%I021 08 The cod0 IVA 4: ModelIn of momentum conawva- tlon In multi-phasa muttlcompom rl! porous madla

flows In hstorogonsous

Kolev, N. 1. Kerntechni&, Nov. 1994, 59, (6), 249-258. The heterogeneous porous body concept together with local volume and time averaging are used to derive rigorously momentum equations for multi-base flows conditionally divided into three velocity fields. All inter- face integrals are suitably transformed in order to enable practical applica- tion. Some minor simplifications are introduced in the finally obtained general equation, and working equations for each of the three velocity fields are recommended for general use in multi-phase fluid dynamic analysis

95K)21% Computstlon of temperatures and atrsssss of fluld- conducting plpss on the bask of the trmpsratun varlatlon on the outer surfaca Sauer, G. Kerntechnic, Nov. 1994, 59, (6), 282-290. (In German) A method for calculating the wall temperature of cylindrical bodies on fhe basis of the temperature variation on the outer surface is presented. The method uses a o-ne-dimensional discretixation of the pipe -wall with heat conducting elements and a modified solution of the equation of heat con- duction. It is shown that the temperature fields can be calculated with a simple finite-clement procedure provided the thermal loads are axisym- metric. The modification of the solution procedure ends up in an alprithm for the time integration of the equation of heat conduction. Additionally, formulas for the calculation of the thermal strurses are given.

%I021 10 Convective heat transfer for cold tubs bundles wlth Ice formatlons In a strsam of watsr st stsady stats Internann, P. A. and Kazmiercxak, M. Int. J. of Heat & Fluid F&w, Dec. 1994, 15, (6). 491-500. Experiments were conducted on cold-tube banks subjected to a cross-flow of water. The tubes were internally cooled below the freezing temperature and became enveloped in ice. The resulting ice shapes, which formed on the outside surfaces of the tubes, were allowed to stabllixc, and their im act on the total steady-state rate of energy exchange between the tubes an : the flowing water was investigated.

%I021 11 Coupling of wall conductlon with natural convsc- tlondominatsd msltlng of a phass change matsrlal J-arooi hf. Numerical Heat Transfer, Part A, Oct. 1994, 26, (4),

Over the’ past decade, solid-liquid phase change in enclosures with natural convection in the liquid base has received increasing research attention. The interest for this prob em stems from its large number of a P lications, among which are energy storage systems using latent heat of &on. The intent of this paper is to report on a computational study of natural convec- tion-dominated melting inside a rectangular enclosure from a vertical wall of finite conductance. A mathematical model is formulated, and a numeri- cal procedure is developed to solve the model quations.

%I02112 Curnnt status of FTIR In the snaiysls of coal rtlUCtUrS Painter. P. et aL. Prenr. Patdm. Cha Sot.. Div. Fuel Chem., 1994.39, (l), 49:63. . ’ - Discusses the Fourier-transform IR spectroscopy as a method for determi- nation of the aliohatic and aromatic contents of coal and coal-derived materials. Topics’include: band assignments, sampling, curve resolution, accuracy, and use of phenolic resins as coal models.

95102113 Datsrmlnatlon of asphaltone solublllty in naphthas Selucky, M. L et al., Fuel, Jan. 1995, 74, (l), 88-91. Thin-layer chromatography with flame-ionixation detection and paper chromatography with densitometric evaluation can be used for determimng relative asphaltene (ASP) solubility in naphthas. While tetrabydrofursn (THF) moves the ASP with the solvent front, the pattern becomes pgres- sively more diffuse and s read along the bed with mcmasing proportions of the tested naphtha in #I e THF eluent. Quantitative evaluation can be achieved using area:slicing of the integrator output and cumulative plotting of the results. Admutures of a known pure precipitant (e.g. n-pentam, n- hexane) can be used for calibration.

142 Fuel and Ensrgy Abstracts March lgN5

(PDF) 95/02109 Computation of temperatures and stresses of fluid-conducting pipes on the basis of the temperature variation on the outer surface - DOKUMEN.TIPS (2024)

FAQs

How do you calculate thermal stress in a pipe? ›

The Formula of Thermal Stress

Original length L0 increase to L. The temperature rise is ^T. L-L0= alpha ^t where alpha is the coefficient of material's linear expansion. L=L0 ( 1+ alpha ^t) So, thermal stress= F/A=Y( L-L0)/L0 where Y is Young's modulus of a material.

What is temperature stress in pipes? ›

Thermal stresses are due to thermal movements of piping and induced stresses by supports and by the surrounding facilities. Piping expands or contracts due to the extreme temperature of the fluid being transported, and due to the temperature difference imposed.

What is the thermal expansion of HDPE pipes? ›

The coefficient of thermal expansion for DriscoPlex® high density polyethylene pipe material is 8.0 x 10-5 in/in/°F. This coefficient results in an approximate expansion for pipe of 1/10/100, that is, 1 inch for each 10°F change for each 100 feet of pipe.

What are the thermal stresses in HDPE water pipes? ›

The stresses caused by these temperature changes given are relatively small. For typical construction practices the stresses range from 255 to 300 psi (1.75 to 2.07 MPa). These stresses are less than 10% of a HDPE yield stress of σyield ≈ 3,500 psi (24 MPa).

What is stress temperature formula? ›

The equation of thermal stress is: Stress =FA = -E a dT, where E is Young's Modulus, a is the coefficient of linear thermal expansion, and dT is the change in temperature.

What is the formula for heat conduction pipe? ›

The heat transfer formula through conduction is given by: Q/t = kA((T1-T2)/l), where Q/t is the rate of heat transfer, k is the thermal conductivity of the material, A is the cross-sectional area, T1-T2 is the temperature difference, and l is the thickness.

What is the formula for thermal expansion of a pipe? ›

ΔL = aLo(T2-T1) (Equation 5)

If the pipe is installed at an ambient temperature of 70 deg F, and the temperature of the pipe increases to 270 deg F, we can expect about 1.5 in of expansion in the 100 ft unanchored run.

What is the temperature of HDPE pipe extrusion? ›

HDPE Pipe Extrusion: Micro-Processes Related to The Air Gap. HDPE used in pipes is a crystalline polymer, which contains 60–80% crystallinity. Processing is carried out at around 200°C, when all the crystalline structures are transformed into an undefined structure as the material exits the die.

What is the temperature limit for HDPE pipe? ›

The low temperature limit is usually regarded as -90°C (130° F). The upper limit temperature for structural and gravity service is 70°C (160° F) for long-term exposure and up to 80°C (180°F) for short-term intermittent exposure..

What is the maximum stress of HDPE? ›

HDPE (High Density Polyethylene) Typical Properties
Physical PropertiesEnglish
Tensile Strength, Ultimate3480 - 6530 psi30 MPa
Tensile Strength, Yield2180 - 4350 psi21.9 MPa
Elongation at Break500 - 1000 %840%
Tensile Modulus116 - 144 ksi0.86 GPa
25 more rows

Which piping material has the highest coefficient of thermal expansion? ›

Piping systems expand and contract with changes in temperature. Thermoplastic piping expands and contracts more than metallic piping when subjected to temperature changes - as much as ten times that of steel.

Does HDPE pipe require thrust blocks? ›

29 Are thrust blocks required with HDPE pipelines? No. HDPE pipe and fittings joined by heat fusion are self-restrained in all applications, and therefore do not require thrust blocks, provided the entire system is fused.

How do you measure thermal stress? ›

To calculate thermal stress:
  • Find the initial and final temperature of the material.
  • Subtract the initial temperature from the final temperature to obtain the temperature difference.
  • Multiply the temperature difference with the coefficient of thermal expansion.
May 9, 2024

How do you calculate pipe stress? ›

Here are the formulas for the hand calculations of piping stress: Internal Pressure Stress: It is calculated by the formula: P * r / t , where 'P' is the internal pressure, 'r' is the inside radius of the pipe, and 't' is the wall thickness.

What is the formula for pipe thermal expansion? ›

ΔL = aLo(T2-T1) (Equation 5)

If the pipe is installed at an ambient temperature of 70 deg F, and the temperature of the pipe increases to 270 deg F, we can expect about 1.5 in of expansion in the 100 ft unanchored run.

What is the thermal stress formula for steel? ›

where α is the coefficient of thermal expansion in m/m°C, L is the length in meter, and Ti and Tf are the initial and final temperatures, respectively in °C. For steel, α = 11.25 × 10–6 / °C. If temperature deformation is permitted to occur freely, no load or stress will be induced in the structure.

Top Articles
Latest Posts
Article information

Author: Aracelis Kilback

Last Updated:

Views: 5873

Rating: 4.3 / 5 (44 voted)

Reviews: 83% of readers found this page helpful

Author information

Name: Aracelis Kilback

Birthday: 1994-11-22

Address: Apt. 895 30151 Green Plain, Lake Mariela, RI 98141

Phone: +5992291857476

Job: Legal Officer

Hobby: LARPing, role-playing games, Slacklining, Reading, Inline skating, Brazilian jiu-jitsu, Dance

Introduction: My name is Aracelis Kilback, I am a nice, gentle, agreeable, joyous, attractive, combative, gifted person who loves writing and wants to share my knowledge and understanding with you.