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Thermal Properties
Thermal Properties, Moisture Diffusivity
Processing and Storage of Ag Products
◦ Heating
◦ Cooling
◦ Combination of heating and cooling
Grain dried for storage
Noodles dried
Fruits/Vegetables rapidly cooled
Vegetables are blanched, maybe cooked and canned
Powders such as spices and milk: dehydrated
Cooking, cooling, baking, pasteurization, freezing, dehydration: all involve heat transfer
Design of such processes require knowledge of thermal properties of material
Continue….Heat is transferred by
Conduction: Temperature gradient exists within a body…heat transfer within the body
Convection: Heat transfer from one body to another by virtue that one body is moving relative to the other
Radiation: Transfer of heat from one body to another that areseparated in space in a vacuum. (blackbody heat transfer)
We’ll consider
Conduction w/in the product
Convection: transfer by forced convection from product to moving fluid
Moisture movement through agricultural product is similar to movement of heat by conduction
Moisture diffusivity
Volume change due to moisture content change
Continue….
Terms used to define thermal
properties
Specific heat
Thermal conductivity
Thermal diffusivity
Thermal expansion coefficient
Surface heat transfer coefficient
Sensible and Latent heat
Enthalpy
Specific Heat
Specific Heat: Specific heat is the quantity of
heat that is gained or lost by a unit mass of
product to accomplish a unit change in
temperature, without a change in state
Units:
◦𝐽
𝑘𝑔°𝐾(SI System)
Conversion of units: 1𝐾𝐽
𝐾𝑔°𝐾= 0.239
𝐵𝑇𝑈
lb°𝐹= 0.239
𝐶𝑎𝑙.
𝑔°𝐾
Specific Heat
Once Specific heat of material is known, then the amount of heat (Q) needed to increase temp. from T1 to T2 is calculated by:
Q = M Cp (T2-T1)Where,
Q = quantity of heat required to change temperature of a mass
Cp = Specific heat at constant pressure
M = mass or weight
Water is a major component of all agricultural products
Cp of water = 4.18 kJ/kg0C
Cp of oils and fats = ½ of Cp of water ………
Cp of grains, powders = ¼ to 1/3 of Cp of water
Cp of ice = ½ Cp of H2O ( therefore, less heat required to raise temp. of frozen product then the same product when it is thawed)
Specific heat
Eq. for calculating Cp based on moisture
Content
SI unit- J/kg K
One calorie equals 4.187 joules
Siebel’s equation for fat free materials
Above freezing Cavg = 3349M + 837.36 J/kgK
Below freezing Cavg = 1256M + 837.36 J/kgK
M- Mass fraction of water (ie. 0.8 or moisture wet basis)
Modified Siebel’s
Above freezing Cavg = 1674F + 837.36 SNF+4186M J/kgK
Below freezing Cavg = 1674.72F + 837.36 SNF+ 2093.4M J/kgK
SNF- solids non fat (fraction)
F – Fat (Fraction)
Based on composition
Heldman and Singh (1981)
Calculate the specific heat for a model
food with the following composition:
carbohydrate 40%, protein 20%, fat 10%,
ash 5%, moisture 25%.
Thermal Conductivity (k)
Measure of ability to transmit heatQ= -k A (dT)
l
K = coefficient of thermal conductivity
For one dimensional heat flow in x direction, k is numerically equal to the quantity of heat (Q) that will flow across a unit cross sectional area (A) per unit of time (t) in response to a temperature gradient of 1 degree per unit distance in x direction
Units:
(SI system) (W/m K)
Thermal Conductivity (k)
k water =0.566 at 0°C
= 0.597 at 20°C
= 0.654 at 60°C
Higher the moisture content higher will be thermal conductivity of food product
Another factor is porosity e.g. freeze dried products and porous fruits like apple have low thermal conductivity.
■ Metals: 50 - 400 W/(m0C)
■Alloys: 10 - 120 W/(m0C)
■Air: 0.0251 W/(m0C) (at 200C)
■ Insulating materials: 0.035 - 0.173 W/(m0C)
Thermal Conductivity (k)
If we don’t know the thermal conductivity, approximate
using...
K = kw Xw + ks(1-Xw)
Where,
Kw =Thermal conductivity of water
Xw= Weight fraction of water
Ks = Thermal conductivity of solids = 0.259 𝑊
m°𝐾
For meats and fish, temperature 0–60C, water
content 60–80%, wet basis, Sweat (1975)
k = 0.08 + 0.52Xw
Estimate the thermal conductivity of hamburger
beef that contains 68.3% water at 20 C.
Given
X m = 0.683
One face of a stainless-steel plate 1 cm thick is
maintained at 110°C, and the
other face is at 90°C. Assuming steady-state
conditions, calculate the rate of heat transfer
per unit area through the plate. The thermal
conductivity of stainless steel is 17 W/(m °C).
Thermal Diffusivity (α)
α quantifies the materials ability to conduct heat relative to its ability to store heat.
α = 𝑘
ρ𝐶𝑝Where,
α = Thermal Diffusivity, Units or m²/s.
k = Thermal conductivity
ρ = density of material
Cp = Specific heat at constant pressure (J/(kg·K)
Example : Estimate the thermal diffusivity of a peach at 22 C. k= 0.57 W/m.K, Cp = 3.6 kJ/kg.K, ρ = 670 kg/m3
Surface heat transfer coefficient (h)
(convective heat-transfer coefficient)When a body is placed in flowing stream of liquid or gas, the body’s temperature will change until it eventually reaches in equilibrium with the fluid. In eq. form also known as Newton’s Law of cooling
𝑑𝑄
𝑑𝑡= h A (Tf- Ts)
Where,
h = surface heat transfer coefficient and has same units as k i.e. 𝑊
m°𝐾Tf = temp. of fluid
Ts = temp of solid body
h depends on fluid velocity, surface characteristics of solids, size and shape of solid and fluid properties ( density and viscosity)
Difficult to tabulate value of h, therefore experimentally determined
Tf
The rate of heat transfer per unit area
from a metal plate is 1000 W/m 2 . The
surface temperature of the plate is 120°C,
and ambient temperature is 20°C.
Estimate the convective heat transfer
coefficient.
Radiation Heat Transfer
Radiation heat transfer occurs between
two surfaces by the emission and later
absorption of electromagnetic waves (or
photons). In contrast to conduction and
convection, radiation requires no physical
medium for its propagation—it can even
occur in a perfect vacuum, moving at the
speed of light,
Liquids are strong absorbers of radiation.
Gases are transparent to radiation, (except
some gases absorb radiation of a particular wavelength (for example, ozone absorbs
ultraviolet radiation).
Solids are opaque to thermal radiation.
Solid materials, such as with solid foods,
our analysis is concerned primarily with
the surface of the material.
All objects at a temperature above 0
Absolute emit thermal radiation.
Thermal radiation emitted from an
object’s surface is proportional to the
absolute temperature raised to the fourth
power and the surface characteristics.
where σ is the Stefan–Boltzmann constant, equal to 5.669 x 10 -8 W/
(m2 K 4); T A is temperature, Absolute; A is the area (m 2); and ε is emissivity,
which describes the extent to which a surface is similar to a blackbody. For
a blackbody, the value of emissivity is 1.
where σ is the Stefan–Boltzmann constant,
equal to 5.669 x 10 -8 W/(m2 K 4);
T A is temperature, Absolute;
A is the area (m 2); and
ε is emissivity,
which describes the extent to which a
surface is similar to a blackbody. For a
blackbody, the value of emissivity is 1.
Calculate the rate of heat energy emitted
by 100 m 2 of a polished iron surface
(emissivity 0.06) as shown in Figure E4.5 .
The temperature of the surface is 37°C.
STEADY-STATE HEAT TRANSFER
In problems involving heat transfer, we
often deal with steady state and unsteady
state (or transient) conditions. Steady-
state conditions imply that time has no
influence on the temperature distribution
within an object, although temperature may
be different at different locations within the
object.
Sensible and Latent heat
Sensible heat: Temperature that can be
sensed by touch or measured with a
thermometer. Temperature change due to
heat transfer into or out of product
Latent heat: Transfer of heat energy with
no accompanying change in temperature.
Happens during a phase change...solid to
liquid...liquid to gas...solid to gas
Latent heat (L)Latent Heat, L, (kJ/kg or BTU/lb)
Heat that is exchanged during a change in phase
Dominated by the moisture content of foods
Requires more energy to freeze foods than to cool foods (90kJ removed to lower 1 kg of water from room T to 0 °C and 4x that amount to freeze food)
420 kJ to raise T of water from 0 ° C to 100 ° C, 5x that to evaporate 1 kg of water
Heat of vaporization is about 7x greater than heat of
fusion (freezing)
Therefore, evaporation of water is energy intensive (concentrating juices, dehydrating foods…)
Latent heat (L)
Determine L experimentally when possible.
When data is not available (no tables, etc) use….
L = 335 Xw where Xw is weight fraction of water
Many fruits, vegetables, dairy products, meats
and nuts are given in ASHRAE Handbook of
Fundamentals
Enthalpy (h)
Units: (J/kg)
Heat content of a material.
Used frequently to evaluate changes in heat content of steam or moist air
Combines latent heat and sensible heat changes
ΔQ = M(h2-h1)
Where,
ΔQ = amount of heat needed to raise temperature from T1 to T2
M = mass of product
h2= enthalpy at temp T1
h1 = enthalpy at temp T2
Enthalpy (h)Approach useful when one of the temperatures is below freezing
Measurements based on zero values of enthalpy at a specified temperature e.g. at -40°C, -18°C or 0°C.
Enthalpy changes rapidly near the freezing point
Change in enthalpy of a frozen food can be calculated from eq. below:
Δh = M cp(T2 –T1) + MXw L
Xw is the mass fraction of water that undergoes phase change(frozen fraction)
L is the latent heat of fusion of water
M is the mass of product
Δh = Change in enthalpy of frozen food
Example
Example 8.3:
Calculate the amount of heat which must be removed
from 1 kg of raspberries when their temperature is
reduced from 25C to -5C.
Assume that the specific heat of raspberries above
freezing is 3.7 kJ/kgC and their specific heat below
freezing is 1.86 kJ/kgC.
The moisture content of the raspberries is 81% and the
ASHRAE tables for freezing of fruits and vegs. Indicate
that at -5C, 27% will not yet be frozen.
Homework Assignment Due
February 20thProblem 1: Determine the amount of heat
removed from 1.5 kg of bologna (sausage)
when cooled from 24C to -7C. Assume MC
of 59% and at -7C, 22% won’t be frozen.
Problem 2: Estimate the thermal diffusivity
of butter at 20°C.