Differential Equations of Cooling Laws

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SUMMARY

The discussion centers on the application of differential equations to model the cooling laws of an electric heater. The equation R = C(dT/dt) + hT is established, where R is the constant heat supply rate, C is the heat capacity, and h is the heat transfer coefficient. Participants explore the integration of this equation, emphasizing the transformation of variables to simplify the integration process. The specific values provided include R = 50 cal/sec, C = 2 cal/deg, and h = 0.04 (cal/sec)/deg, which are used to derive T in terms of t.

PREREQUISITES
  • Understanding of differential equations
  • Familiarity with Newton's law of cooling
  • Knowledge of heat transfer concepts
  • Basic calculus skills for integration
NEXT STEPS
  • Learn how to solve first-order linear differential equations
  • Study the method of separation of variables in differential equations
  • Explore applications of Newton's law of cooling in real-world scenarios
  • Investigate the impact of varying heat transfer coefficients on cooling rates
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Students studying thermodynamics, physics enthusiasts, and anyone interested in the mathematical modeling of heat transfer processes.

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Homework Statement


When you turn on an electric heater, such as "burner" on a stove, its temperature increases rapidly at first, then more slowly, and finally approaches a constant high temperature. As the burner warms up, heat supplied by the electricity goes to two places.
i.) Storage in the heater materials, thus warming the heater
ii.) Losses to the room
Assume that heat is being supplied at a constant rate, R. The rate at which heat is stored is directly proportional to the rate of change of temperature. Let T be the number of degrees above room temperature. Let t be time in seconds. Then the storage rate is C(dT/dt). The proportionality constant, C (calories per degree), is called the heat capacity of the heater materials. According to Newton's law of cooling, the rate at which heat is lost to the room is directly proportional to T. The (positive) proportionality constant, h, is called the heat transfer coefficient.

a.) The rate at which heat is supplied to the heater is equal to the sum of the storage rate and the loss rate. Write a differential equation that expresses this fact.
b.) Separate the variables and integrate the differential equation. Explain why the absolute value sign is not necessary in this case. Transform the answer so that temperature, T, is in terms of time, t. Use the initial condition that T=0 when t=0.
c.) Suppose that heat is supplied at a rate, R=50 cal/sec. Assume that the heat capacity is C=2 cal/deg, and that the heat transfer coefficient is h=.04 (cal/sec)/deg. Substitute these values to get T in terms of t alone.


Homework Equations



dT/dt = k(M - T)

The Attempt at a Solution



Part a)

R = C (DT/dt) + hT

Part b)

R - hT = C(dT/dt)
→(R - hT) dt = C(dT)
→ ∫(R-hT) dt = ∫ C dT



Please tell me if I did it correctly, and help me integrate.

Thanks!


Same problem, but topic was locked:
https://www.physicsforums.com/showthread.php?t=277738
 
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R = C (dT/dt) + hT

should be
R = C (dT/dt) + h(T-Ts)
where Ts is the surrounding temperature, it does say we can assume T=0 though

now when you integrate, you attempt to separate variables, this essentially means you try and get all the T's on one side and all the t's on the other
R-hT= C \frac{dT}{dt}

This is complicated by the R term, so to seperatre and inetgrate, I would do the follwing transform first, let
U = hT-R
then
\frac{dT}{dt}=\frac{1}{h}\frac{dU}{dt}

now the equation is separable and it should be simpler to integrate, then you can transform back to T at the end
-U= \frac{C}{h} \frac{dU}{dt}
 

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