Thick versus Thin Wall Pipes

Before we combine all forms of heat transfer, one last distinction should be made about the surface area of heat transfer in pipes.

The area used in a heat transfer calculation should be the area that the heat transfer is taking place. In a thin walled pipe, the difference in area of the inside of the pipe to the outside of the pipe is rather close. However, in a thick walled pipe, such as a pipe with insulation, the surface area of heat transfer will change from the centre of the pipe to the outside. For this reason, in thick walled pipes the area used is the log mean area of the pipe, defined as:

A subscript L M end subscript equals 2 pi L fraction numerator left parenthesis r subscript 2 minus r subscript 1 right parenthesis over denominator ln space left parenthesis begin display style r subscript 2 over r subscript 1 end style right parenthesis end fraction

Where L is the length of the pipe and the inner and outer radii of the pipe are r1 and r2 respectively.

Let us do an example involving a thick wall pipe.

Steam at 170°C flows through a 100 m length insulated pipe. The pipe ID is 150 mm and the pipe thickness is 7.5 mm. The insulation is 50 mm thick with a thermal conductivity of 0.073 Wm-1 K-1. The surface temperature of the insulation is 37°C.  

Calculate the rate of conduction through the insulation.

To solve this problem, we will first draw a schematic to better illustrate the scenario.

Figure: Conduction through insulated steam pipe

Figure: Conduction through insulated steam pipe

We will use the overall heat transfer equation to solve for the rate of heat transfer via conduction.

q equals U A capital delta T

The thermal resistance of both the inside condensing film coefficient of steam and the wall of the pipe will be negligible compared to the insulation so we can ignore those terms in the determination of U. So, we can simplify to:

q equals k over x space A capital delta T

The area of heat transfer will be the log mean surface area of the pipe.

A subscript L M end subscript equals 2 pi L fraction numerator left parenthesis r subscript 2 minus r subscript 1 right parenthesis over denominator ln space left parenthesis begin display style r subscript 2 over r subscript 1 end style right parenthesis end fraction

The length of the pipe is given as 100 m.

r1 is the distance from the inside of the steam pipe to the outside of the steam pipe.

r subscript 1 equals 150 over 2 plus 7.5 equals 82.5 m m equals 0.0825 m

r2 is the distance from the inside of the steam pipe to the outside of the insulation.

r subscript 2 equals 150 over 2 plus 7.5 plus 50 equals 132.5 m m equals 0.1325 m

Now we need to calculate the area.

A subscript L M end subscript space equals space 2 pi space cross times space 100 space cross times space fraction numerator left parenthesis 0.1325 minus 0.0825 right parenthesis over denominator ln space left parenthesis begin display style fraction numerator 0.1325 over denominator 0.0825 end fraction end style right parenthesis end fraction

A subscript L M end subscript space equals space 66.3 space m squared

Finally, we can calculate the conductive heat transfer rate. 

q equals fraction numerator k over denominator x space end fraction A capital delta T

q equals fraction numerator 0.073 over denominator 0.05 end fraction space cross times space 66.3 space cross times space left parenthesis 37 minus 170 right parenthesis

q equals negative 12 comma 874 space W equals negative 12.9 space k W

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