BULETINUL INSTITUTULUI POLITEHNIC DIN IAŞI

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74 Bogdan Horbaniuc et al cooling extracts heat from the region in the vicinity of the tube, the SSM layers located far from the tube continue to transmit heat to the regions farther away, until they are reached by the thermal perturbation. This explains why the temperature plots continue to advance towards the end of the SSM domain, although a cooling occurs at the other end. Fig. 4 – The amount of stored heat versus time during charging. Fig. 5 – The amount of stored heat versus time during charging.
Bul. Inst. Polit. Iaşi, t. LVIII (LXII), f. 3, 2012 75 Fig. 6 – Temperature field evolution during the discharging process. A 3-D view of the temperature field evolution similar to that of Fig. 4 is represented in Fig. 7. In the case of discharging, a plot similar to that from Fig. 5 is less significant in terms of information offered. Fig. 7 – 3-D surface representation of the temperature field during discharging.
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BULETINUL INSTITUTULUI POLITEHNIC D
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BULETINUL INSTITUTULUI POLITEHNIC D
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PETRU CÂRLESCU, VASILE DOBRE, IOAN
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2 Niooleta Negoescu continue telle
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4 Niooleta Negoescu min{ μ( Tu , T
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6 Niooleta Negoescu Observation 8.
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BULETINUL INSTITUTULUI POLITEHNIC DIN IAŞI

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