Spatial Effects QUESTION: When can we neglect the temperature variation inside a solid? We can do that if the heat transfer via conduction inside the solid.

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Presentation transcript:

Spatial Effects QUESTION: When can we neglect the temperature variation inside a solid? We can do that if the heat transfer via conduction inside the solid is much more effective than heat transfer via convection between the solid and the ambient fluid. This can be demonstrated as follows: Heat transfer from the fluid to the solid through convection: q=hA(TS-T) and the thermal resistance of this process is Rconv=1/(hA). Heat transfer from the exterior of the solid to the interior of the solid is through the conductive heat transfer: YAC 8-6

Biot Number In order to be able to use the lumped capacitance assumption, the temperature variation inside the solid should be much smaller than the temperature difference between the surface and the fluid: TS-T << TS,1-TS,2. In other words, the thermal convection resistance should be much greater than the thermal conduction resistance. Rconv>>Rsolid.

Biot and Fourier Numbers Define Biot number Bi=hLC/k In general, Bi<0.1 for the lumped capacitance assumption to be valid.

Spatial Effects Re-examine the plasma jet example: h=30,000 W/m2.K, k=10.5 W/m.K, and a diameter of 50 mm. Bi=(h/k)(rO/3)=0.0238<0.1. Therefore, the use of the LCM is valid in the previous example. However, if the diameter of the particle is increased to 1 mm, then we have to consider the spatial effect since Bi=0.476>0.1. The surface temperature can not be considered as the same as the temperature inside the particle. To determine the temperature distribution inside the spherical particle, we need to solve the unsteady heat equation:

Transient Conduction in Plane Walls. Cylinders & Spheres Heisler Charts show the non-dimensional Temp. distributions, the Max. temperatures and the total Heat transfer

Example Problem Recalculate the plasma jet example by assuming the diameter of the particles is 1 mm. (a) Determine the time for the center temperature to reach the melting point, (b) Total time to melt the entire particle. First, use the lumped capacitance method and then compare the results to that determined using Heisler charts. (h=30000 W/m2, k=10.5 W/m.K, r=3970 kg/m3, rO=0.5 mm, cP=1560 J/kg.K, T=10000 K, Ti=300 K, Tmelt=2318 , hsf=3577 kJ/kg, a=k/(rcP)=1.69510-6(m2/s). First, Bi=(h/k)(rO/3)=0.476>0.1 should not use LCM. However, we will use it anyway to compare the difference.

Example Problem (cont’d)

Heisler Chart Note: this is the magnified upper left corner of Fig. 9-15 O*=0.792 Bi-1=0.7 t*=t t*=0.16=at/rO2 t=(rO2/a)(0.16)=0.023(s) much longer than the value calculated using LCM (t=0.008 s)

Approximate Solution

Heat Transfer 0.48 6 8 2 3 4 5 Bi=1.428 0.353

Heat Transfer (cont.) Total heat transfer during this period: Q=Qmax(Q/Qmax)=31438(0.48)=15090(J) The actual process is more complicated than our analysis. First, the temperature will not increase once the solid reaches the melting temperature unless the solid melts into liquid form. Therefore, the actual heat transfer process will probably slower than the estimation. If the outer layer melts then we have double convective conditions: convection from the plasma gas to the liquid alumina and then from there to the inner solid. To make matter even more complicated, the interface between the melt alumina and the solid is continuously moving inward. No analytical solutions or numerical analysis is necessary.