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Overall Heat Transfer Coefficient in Heat Exchangers

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Overall Heat Transfer Coefficient in Heat Exchangers

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Rohit Abudhia
Rohit Abudhiastudent
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Article details

Heat exchangers play a critical role in many industrial processes by enabling the efficient transfer of heat between two fluids at different temperatures. One of the most important parameters in the design and analysis of heat exchangers is the overall heat transfer coefficient (U), which quantifies the efficiency of heat transfer across all barriers separating the fluids.

1. Heat Transfer Mechanism in Heat Exchangers

In a typical heat exchanger, two fluids—one hot and one cold—are separated by a solid wall. The heat transfer process involves multiple steps:

  1. Heat is first transferred from the hot fluid to the wall by convection.

  2. Heat then moves through the wall by conduction.

  3. Finally, heat is transferred from the wall to the cold fluid by convection again.

Radiation is usually negligible and incorporated into the convection coefficients if needed.

2. Thermal Resistance Concept

To analyze heat exchangers effectively, the concept of thermal resistance is introduced. The resistance of the solid wall to heat conduction is calculated by:

                                                   

Where:

  • Do and Di are the outer and inner diameters of the wall.

  • k is the thermal conductivity of the wall material.

  • L is the length of the heat exchanger.

The total thermal resistance, considering convection on both sides and conduction through the wall, is expressed as:

                    

Where:

  • hi and ho are the convective heat transfer coefficients for the inner and outer surfaces.

  • Ai and Ao are the respective surface areas.

3. Overall Heat Transfer Coefficient

The overall heat transfer coefficient UU provides a convenient way to combine these resistances into a single term that governs the rate of heat transfer QQ:

                 

Where:

  • A is the appropriate surface area (inner or outer).

  • (ΔT)Delta T is the temperature difference between the hot and cold fluids.

By rearranging and simplifying the resistances, the expression for U becomes:

                  

When the wall is very thin and highly conductive (i.e., Rwall is negligible), the equation simplifies to:

                                                         

This formula is particularly useful for many practical applications where wall resistance is small compared to convective resistances.

4. Practical Implications

In cases where one fluid has a much smaller convection coefficient than the other (e.g., gas vs. liquid), the smaller coefficient dominates the overall heat transfer rate. This is because:

                                                       

This creates a bottleneck in the heat transfer path and significantly reduces heat exchanger efficiency. Engineers must carefully consider this when designing systems, especially when gas-liquid interfaces are involved.

 

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