When to use the Lumped Capacitance method in Heat Transfer problems?

In summary, the main assumption for applying the lumped capacitance method is that the external resistance dominates over the internal resistance to heat at long times. This can be represented by the Biot number, which is the ratio of the internal resistance (k/L) to the external resistance (1/h). The nominator (k/L) represents the internal resistance while the denominator (1/h) represents the external resistance. The method is considered valid when the Biot number is much smaller than 1, or when Bi << 1.
  • #1
Sabra_a
33
6
Homework Statement
What is the main assumption to apply the lumped capacitance method? What particular non dimensional number and what mathematical condition represent this assumption? What is the meaning of the nominator and the denominator in this non-dimensional number?
Relevant Equations
Energy released
Biot number
I attached below my attempt to solve the question.
Screen Shot 2019-12-20 at 2.01.35 PM.png
Screen Shot 2019-12-20 at 2.02.10 PM.png
 
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  • #2
Sabra_a said:
Homework Statement:: What is the main assumption to apply the lumped capacitance method? What particular non dimensional number and what mathematical condition represent this assumption? What is the meaning of the nominator and the denominator in this non-dimensional number?
Relevant Equations:: Energy released
Biot number

I attached below my attempt to solve the question.
View attachment 254413View attachment 254414
In a system like this, the asymptotic internal resistance to heat at long times is proportional to L/k and the external resistance is proportional to 1/h. The lumped parameter approach is valid if the external resistance dominates, or when $$\frac{1}{h}>>\frac{L}{k}$$or when $$\frac{k}{Lh}>>1$$ or, equivalently, when Bi << 1.
 

1. What is the Lumped Capacitance method in Heat Transfer?

The Lumped Capacitance method is a simplified approach to solving heat transfer problems where the temperature of a solid object changes due to a sudden change in its surroundings. It assumes that the object can be treated as a single lumped capacitor with a uniform temperature distribution.

2. When is it appropriate to use the Lumped Capacitance method?

The Lumped Capacitance method is appropriate to use when the Biot number (Bi) is less than 0.1. This means that the heat transfer at the surface of the object is much faster than the heat transfer within the object. It is also suitable for short-duration processes where the temperature change is significant within a short period of time.

3. What are the limitations of the Lumped Capacitance method?

The Lumped Capacitance method has several limitations, including the assumption of a uniform temperature distribution in the object, neglecting the internal temperature gradients, and not accounting for convection or radiation effects. It is also not suitable for long-duration processes where the temperature change is gradual.

4. How accurate is the Lumped Capacitance method?

The accuracy of the Lumped Capacitance method depends on the assumptions made and the conditions of the problem. It can provide reasonable results for short-duration processes with low Biot numbers. However, for more complex and longer processes, it may not accurately capture the temperature distribution within the object.

5. Can the Lumped Capacitance method be used for all heat transfer problems?

No, the Lumped Capacitance method is only applicable to certain types of heat transfer problems, specifically those with low Biot numbers and short-duration processes. It is important to carefully consider the conditions and assumptions before deciding to use this method for a particular problem.

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