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When Bernoulli's theorem is expressed as
\( \mathrm{P} \)
\[
\frac{P}{\rho g}+\frac{1}{2} \frac{v^{2}}{g}+h=\text { constant }
\]
W
the dimensions of the constant on the right hand side of the equation are given as
(1) \( \quad \mathrm{M}^{0} \mathrm{~L}^{0} \mathrm{~T}^{0} \)
(2) \( \quad \mathrm{M}^{0} \mathrm{~L}^{1} \mathrm{~T}^{0} \)
(3) \( \mathrm{M}^{1} \mathrm{~L}^{0} \mathrm{~T}^{0} \)
(4) \( \mathrm{M}^{1} \mathrm{~L}^{2} \mathrm{~T}^{-2} \)
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