Timothy Jackman, Matthew Barg, Emily Peterson ME 340.

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Timothy Jackman, Matthew Barg, Emily Peterson ME 340

description

 1 Electric 450 K (350°F)  1 Thermocouple  1 Timer

Transcript of Timothy Jackman, Matthew Barg, Emily Peterson ME 340.

Page 1: Timothy Jackman, Matthew Barg, Emily Peterson ME 340.

Timothy Jackman, Matthew Barg, Emily PetersonME 340

Page 2: Timothy Jackman, Matthew Barg, Emily Peterson ME 340.

We were interested in verifying the accuracy of the lumped capacitance model for steak, chicken, and hamburger.

Page 3: Timothy Jackman, Matthew Barg, Emily Peterson ME 340.

1 Electric Oven @ 450 K (350°F) 1 Thermocouple 1 Timer

Page 4: Timothy Jackman, Matthew Barg, Emily Peterson ME 340.

Air @ 450 K ρ = 0.774 kg/m3

cp= 1.021 KJ/kg K μ = 250.7 E-7 N

s/m2

ν = 32.39 E-6 m2/s k = 37.3 E-3 W/m K α = 47.2 E-6 m2/s Pr = .686 β = 2.22 E-3 K-1

T1-T2 = 290 K

RaL = gβ(T1-T2)L3/αν

RaL = (9.81)(2.22 E-3)(290)(0.432)3

(47.2 E-6)(32.39 E-6)

RaL = 3.327 E8

Ћ = k(0.069RaL 1/3)(Pr0.074)/L

Ћ = (37.3 E-3)(0.069)(3.327 E8)1/3(0.686)0.074/0.432

Ћ = 4.01 W/m2 K

We measured the temperature difference between the top and bottom coils in the oven and used Incropera equation 9.49 to determine the convective coefficient.

Page 5: Timothy Jackman, Matthew Barg, Emily Peterson ME 340.

  Density (kg/m3) Cp (kJ/kg K) k (W/m K)

Steak 1,234 3.005 0.480

Hamburger 1,015 3.005 0.380

Chicken 1,000 1.560 0.489

Page 6: Timothy Jackman, Matthew Barg, Emily Peterson ME 340.

Our goal was to compare the actual temperature increase in the meat over eight minutes compared to the estimated temperature increase using Lumped Capacitance.

Page 7: Timothy Jackman, Matthew Barg, Emily Peterson ME 340.

We measured the initial temperature of the meat and placed it in the oven at constant temperature.

After eight minutes, we measured the internal temperature of the meat at the center.

Page 8: Timothy Jackman, Matthew Barg, Emily Peterson ME 340.

Lumped Capacitance is a valid model. Incropera equation 9.49 is valid:

Convective coefficient model was valid for L/H << 1, while our L/H = 17/22.

We assumed the temperature difference in the coils was the temperature difference of the enclosure.

The oven was at a constant temperature.

Page 9: Timothy Jackman, Matthew Barg, Emily Peterson ME 340.

Calculate the Biot number to confirm that Lumped Capacitance can be used.Bi = ЋLc/k

Bisteak = 0.051

Bihamburger = 0.081

Bichicken = 0.051

Bi < 0.1 so lumped capacitance may be used for all meats

Page 10: Timothy Jackman, Matthew Barg, Emily Peterson ME 340.

T(t) = T∞ + (To - T∞)exp(-ЋAst/ρcpV)

For chicken:

T(480s) = 450 + (290-450)exp[-(480)(4.01)(1.508 E-2)/(1000)(1.560)(9.29 E-5)]

T(480s) = 322.2 K

Page 11: Timothy Jackman, Matthew Barg, Emily Peterson ME 340.

Steak Hamburger ChickenTo (K) 290 289.9 290

V (m3) 9.07E-05 7.68E-05 9.30E-05

As (m2) 0.0148 9.99E-03 1.51E-02

Tmeasured (K) 319 324.5 322.2

Tcalculated (K) 301 302 319

error (%) 5.7 6.9 1.0

Page 12: Timothy Jackman, Matthew Barg, Emily Peterson ME 340.

Lumped capacitance accurately predicted the temperature of the meats after 8 mins.

Error of 1–6.9% was obtained from this experiment.