22-Agric-B8 Food Process Engineering (Part 1) · December 2013
Question 7 of 10: Freezing Time in Liquid Nitrogen — Surface Heat Transfer Coefficient
Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
Notes on this paper
Paper format. 04-Agric-B8 Food Process Engineering (Part 1), National
Exams December 2013 — a three-hour open-book exam (any non-communicating
calculator permitted). Ten questions are set in four sections (I–IV), each with a
"choose N of M" instruction; candidates who follow the choice rule answer six questions for a
100-mark paper. All ten are worked here so the set is a complete study resource.
Reference texts. R.T. Toledo, Fundamentals of Food Process Engineering,
3rd ed. (thermal-process lethality, D and z values, Ball/Stumbo process calculation, aseptic
holding-tube residence time — this is the exam's own appendix source); C.J. Geankoplis,
Transport Processes and Separation Process Principles, 4th ed. (evaporator heat and
mass balances, multiple-effect steam economy, vapour recompression); R.P. Singh and
D.R. Heldman, Introduction to Food Engineering, 5th ed. (freezing-time estimation,
modified Plank equation, unsteady-state heat transfer in canned foods); A.C. Cleland,
Food Refrigeration Processes: Analysis, Design and Simulation (Plank/Cleland-Earle
freezing-time correlations); F.P. Incropera and D.P. DeWitt, Fundamentals of Heat and Mass
Transfer (transient conduction, Heisler charts, composite-wall resistance).
Question 7: Freezing Time in Liquid Nitrogen — Surface Heat Transfer Coefficient (15 marks)
Find. The surface convective heat transfer coefficient, \(h\).
Immersion freezing modelled as an infinite slab, cooled from both faces.
Approach. Get the total heat removed per kg of product from an energy balance
on the nitrogen itself (it boils off at -196°C, then the cold gas warms toward ambient,
absorbing sensible heat too); back out the cake's bulk density from its mass and geometry; solve
the modified Plank equation (infinite slab, \(P=\tfrac12\), \(R=\tfrac18\), with \(\Delta H\)
replacing the pure latent heat to also cover the pre- and sub-cooling sensible loads) for \(h\).
Total heat removed per kg product, from the nitrogen side. Each kg of N2
absorbs its latent heat at -196°C, then the resulting cold gas is credited with warming back
to the 22°C ambient (a standard LN2 mass-balance shortcut, since the vented gas ultimately
equilibrates with the room): \(\Delta h_{N_2} = L_{N_2}+c_{p,N_2}(T_{amb}-T_{N_2})
=197.98+1.044(22-(-196))=\boxed{425.6\ \text{kJ/kg N}_2}\).
Per kg product: \(\Delta H = 0.665\times425.6=\boxed{283.0\ \text{kJ/kg product}}\).
Modified Plank equation, solved for \(h\). With \(a=0.04\) m (full slab
thickness), \(P=\tfrac12\), \(R=\tfrac18\), \(T_f-T_m=-2-(-196)=194\ \text{K}\):
\(t=\dfrac{\rho\Delta H\,a}{T_f-T_m}\left(\dfrac{P}{h}+\dfrac{Ra}{k}\right)\).
The conduction term alone accounts for \(37.7\ \text{s}\) of the 102 s total, leaving the
surface term to supply the rest; solving,
\(\boxed{h \approx 101.6\ \text{W/(m}^2\text{K)}}\).
Final results
Quantity
Value
Cake bulk density
223.8 kg/m³
Total heat removed per kg product
283.0 kJ/kg
Surface heat transfer coefficient, \(h\)
≈ 101.6 W/(m²·K)
Check: crediting the vented nitrogen gas with warming fully to ambient
(22°C) before leaving the freezing tunnel is the standard textbook shortcut for this class of
problem; a real tunnel recovers less of that sensible enthalpy, which would lower \(\Delta H\)
per kg product and hence lower the back-calculated \(h\) somewhat. The resulting \(h\approx
100\ \text{W/(m}^2\text{K)}\) sits in the expected range for LN2 immersion/spray freezing.