Bernoulli’s theorem describes the conservation of energy in a flowing fluid and can be derived by analyzing the work done by pressure forces, gravity, and changes in velocity along a streamline. It is mathematically expressed as:
\[
P + \rho gh + \frac{1}{2} \rho v^2 = \text{constant},
\]
where:
\( P \): Pressure energy per unit volume,
\( \rho \): Density of the fluid,
\( g \): Gravitational acceleration,
\( h \): Height above a reference level,
\( v \): Velocity of the fluid.
To analyze the given options:
Option (a): The use of \( m \) (mass) instead of \( \rho \) (density) is incorrect because Bernoulli’s equation is based on energy per unit volume, not mass.
Option (c): Modifying the potential energy term as \( mg \) instead of \( \rho gh \) is dimensionally inconsistent.
Option (d): Changing the kinetic energy term from \( \frac{1}{2} \rho v^2 \) to \( \frac{1}{2} m v^2 \) is incorrect for fluid dynamics, as it does not conform to energy per unit volume.
Only option (b) correctly preserves the balance of energy terms per unit volume:
\[
P + \rho gh + \frac{1}{2} \rho v^2 = \text{constant}.
\]
Final Answer:
\[
\boxed{P + \rho gh + \frac{1}{2} \rho v^2 = \text{constant}}
\]