Steam Tracing Appendix
Steam Tracing Appendix
Steam Tracing Appendix
Heat tracing is used to prevent heat loss from process fluids being transported in process fluid pipes, when there is risk of damage to piping, or interference with operation such as fouling or blockage, caused by the congealing, increase in viscosity, or separation of components in the fluid below certain temperatures, or when there is risk of formation of corrosive substances or water due to condensation in corrosive services. This prevention of heat loss is accomplished by employing electrical tracing or steam tracing, and insulating both the process fluid pipe and the tracer together, using appropriate insulation lagging, in an attempt to minimise heat loss from the pipe and tracer to their surroundings. Steam tracing is described by attaching a smaller pipe containing saturated steam, also known as the tracer, parallel to the process fluid pipe. The two pipes are then also insulated together with the specified insulation and jacketed if necessary. Steam tracing is more labor intensive to install than electrical heat tracing, but there are very few risks associated with it. The temperature of the tracer also cannot exceed the maximum saturation temperature of the steam, as it operates at specific steam pressures. Steam tracing may be done in one of two ways. Bare steam tracing is the most popular choice as it is fairly easily installed and maintained and it is ideally suited to lower temperature requirements. It is simply composed of a half inch or three quarters of an inch pipe containing saturated steam attached to the process fluid pipe by straps and both pipes are then insulated together. The other available option is to make use of cemented steam tracing, during which heat conductive cement is placed around the steam tracer running parallel to the process fluid pipe, (shown in figure 1b), in an attempt to increase the contact area available for heat transfer, between the tracer and the process fluid pipe. Because the area around the process fluid pipe and tracer cannot be accurately described simply by assuming perfect cylindrical geometry, provision had to be made for a realistic impression of the true geometry. (See figures 1a and 1b)
For bare tracing, the following formulas were derived: The calculations for the cemented tracer are not shown, but are derived from the same principles
= cos 1
r1 r2 r1 + r2
tan =
Lai (r1 r2 )
with 2Lai being the area of annulus space exposed to insulation per metre of pipe length, and r1 and r2 being the outer diameters of the process fluid pipe and the steam tracer pipe, respectively.
Circumference = 2r2
1 4
Q pl =
L(T p Tamb )(2 (1.25 + 0.75n ) ) r1 ln r1( inner ) kw ln rins + r1 k ins + 1 ho rins
ho =
q = 0.548
W/m2
) (
5 4
2.85Vm + 1
Tsurf
low
Tsurf
hottest
It was assumed that 80% of the surface temperature is contributed by Tsurf, low, the surface temperature on the process fluid side of the pipe, and 20% of the surface temperature is contributed by the surface temperature on the steam line side of the pipe, which is also the hottest surface temperature.
Q = Qtl + Qal + Q pl
References Le Roux, D.F. (1997) Thermal Insulation and Heat Tracing, Guideline presented by line manager D.F. le Roux, Secunda. Foo, K.W. (1994) Sizing tracers quickly (Part 1). Hydrocarbon Processing, p93-97. January. Sizing tracers quickly (Part 2). Hydrocarbon Processing, p93-97. February. Fisch, E. (1984) Winterising process plants. Chemical Engineering, p128-143, 20 August. Kenny, T.M. (1992) Steam tracing: do it right. Chemical Engineering Progress, p40-44, August. Coulson, J.M and Richardson, J.F. (1999) Chemical Engineering, R.K. Sinnot, London. Le Roux, D.F. (2005) Theoretical discussion and problem description, Sasol Limited, Secunda. Van der Spuy, E. (2005) Theoretical advice, and steam traps, Spirax Sarco, Secunda. Smit, J. (2005) Practical information, Sasol Limited, Secunda. Technical committee of specification SP 50-4, (2004) Specification SP 50-4 Revision 2 for Steam and Hot Water Tracing, Sasol Limited, Secunda.
= cos 1
tan =
r1 r2 r1 + r2
Lai (r1 r2 )
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Energy added by tracer Energy lost by system: Refer again to Fig. 3a.
The movement of energy across the system boundaries may be explained as follows: Qta + Qtp + Qtl = Qtl + Qal + Q pl
Qtp 0
Qta = Qal + Q pl
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The convection heat transfer coefficient for the annulus (still air) is given by
T Tann 4 hc = 1.18 s Le Roux, D.F. (1997) Thermal Insulation and Heat 2r2 Tracing, Guideline presented by line manager D.F. le Roux, Secunda.
The remaining design equations for bare tracing are given in section 4.:Results and Discussion.
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= cos 1
sin =
r1 r2 r1 + r2
Lact =
tan (r1 r2 )
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Energy added by tracer Energy lost by system: Refer again to Fig. 3b.
The energy movement across the system boundaries may be explained as follows: Qca + Qcp + Qcl = Qcl + Qal + Q pl
Qca + Qcp = Qal + Q pl Aca = nL(0.2357 Dt 2 (r2 + ct )) Acp = 4nLr2 Molloy, J.F., Fundamentals of Heat Transfer, p72 101 rins r1 A pl = L (2 (1.25 + 0.75n ) ) rins ln r 1 The remaining equations are given in section 4:Results and Discussions.
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