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Shell-and-Tube Heat Exchangers - Cheresources.com

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2⎛G⎞t∆ Pr= 4 × Number of tube passes ×⎜ ⎟⎝2ρ⎠Here,Gt= ρ V is the mass velocity <strong>and</strong> is defined asMass flow rate mGt=Total flow area available per pass At<strong>and</strong>A tTotal number of tubes × Cross -sectional area of a tube=Number of passes<strong>Shell</strong>-Side Pressure DropThere are several ways to estimate the pressure drop for the flow of the shell-side fluid in a shell<strong>and</strong>-tubeheat exchanger. A reasonable estimate can be obtained by the relatively simpleapproach described below, which is given in a book by Peters, Timmerhaus, <strong>and</strong> West (2). Thisbook also provides much valuable information on the design of such heat exchangers, includingmore sophisticated methods of estimating the pressure drop.The pressure drop on the shell-side is calculated using∆ P =shellfGD( N + )22s s B10.14⎛ρD µ ⎞e ⎜ ⎟⎝µs ⎠In this equation, f is a Fanning friction factor for flow on the shell side given in Figure 14-44 ofreference (2), Gsis the mass velocity on the shell side, Dsis the inside diameter of the shell,NBis the number of baffles, ρ is the density of the shell-side fluid, <strong>and</strong> Deis an equivalentdiameter. The mass velocity Gs= m/Sm, where m is the mass flow rate of the fluid, <strong>and</strong> Smisthe crossflow area measured close to the central symmetry plane of the shell containing its axis.This area is defined asclearanceCross flow area = DsLB×pitchwhereBL is the baffle spacing, <strong>and</strong> the clearance <strong>and</strong> pitch are defined in the notes on shell-<strong>and</strong>tubeheat exchangers. The equivalent diameter is defined as follows.8

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