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Gas Turbine Handbook : Principles and Practices

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Appendix C 381<br />

Solving for CDT yields 886°F.<br />

At 95% <strong>and</strong> 100% RH the air flow into the gas turbine includes 16.6<br />

pps of water. At a latent heat of vaporization of 970 Btu/# this water<br />

will give up 16,050 Btu/sec (cp = 0.24672).<br />

Using Q = W A<br />

• c p<br />

• ∆T<br />

Solving for ∆T yields 130°F.<br />

Therefore, the dry bulb temperature of 886°F will be reduced to<br />

756°F.<br />

This addresses the maximum amount of water that can be expected<br />

to be evaporated in the inlet system upstream of the gas turbine-compressor<br />

inlet. Now consider adding water for wet compression.<br />

Consider first adding 90 gpm of water to this inlet condition. This is<br />

approximately 2.5% of the inlet flow.<br />

Within the compressor this water is evaporated through latent heat<br />

of evaporation.<br />

At 90 gmp = 12.5 pps; then 12.5 pps ⋅ 970 Btu sec<br />

= 12,125 Btu/sec Heat Absorbed<br />

Again solving for ∆T yields 99°F. Therefore, the injection of 90 gpm<br />

into the air stream at the compressor inlet will result in a compressor<br />

discharge temperature of 656°F.<br />

Increasing amounts of water can be added until either the compressor<br />

surges or the discharge from the compressor contains liquid water<br />

droplets.<br />

Consider adding 10% water at the original inlet conditions.<br />

10% water = 50 pps = 360 gpm.

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