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Saturated vapour is condensed to saturated liquid in a condenser. The heat capacity ratio is \(C_{r} = \frac{C_{min}}{C_{max}}\). The effectiveness (∈) of the condenser is :

  • A.\(1 - \exp(-\text{NTU})\)
  • B.\(\frac{1 - \exp[-\text{NTU}(1 + C_{r})]}{1 + C_{r}}\)
  • C.\(\frac{1 - \exp[-\text{NTU}(1 - C_{r})]}{1 + C_{r}[-\text{NTU}(1 - C_{r})]}\)
  • D.\(\frac{\text{NTU}}{1 + \text{NTU}}\)

Answer: A

The effectiveness is \(1 - \exp(-\text{NTU})\).

In a condenser the condensing vapour stays at its saturation temperature while it gives up latent heat, so its effective heat capacity rate is infinite. That makes \(C_{max} \to \infty\), and so the capacity ratio \(C_{r} = C_{min}/C_{max} = 0\).

Putting \(C_{r} = 0\) in any of the standard effectiveness relations, parallel or counter flow, gives the same result:

\[ \varepsilon = 1 - e^{-\text{NTU}} \]

Option B is the parallel-flow relation, which reduces to this only when \(C_{r} = 0\); option C is a garbled counter-flow form; and \(\frac{\text{NTU}}{1 + \text{NTU}}\) is the counter-flow result for \(C_{r} = 1\), the opposite limit.

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