The Bernoulli's equation for adiabatic process and compressible flow is
1
\(\left( {\frac{K}{{K - 1}}} \right)\frac{p}{{\rho g}} + \frac{{{V^2}}}{{2g}} + z = \) constant
2
\(\left( {\frac{{K - 1}}{K}} \right)\frac{p}{{\rho g}} + \frac{{{V^2}}}{{2g}} + z = \) constant
3
\(\left( {K-1} \right)\frac{p}{{\rho g}} + \frac{{{V^2}}}{{2g}} + z = \) constant
4
\(\left( K \right)\frac{p}{{\rho g}} + \frac{{{V^2}}}{{2g}} + z = \) constant