This equation was obtained by integrating the Euler’s equation (the equation of motion) with respect to a displacement ‘ds’ along a streamline. Thus, the value of C in the above equation is constant only along a streamline and should essentially vary from streamline to streamline.

The equation can be used to define relation between flow variables at point B on the streamline and at point A, along the same streamline. So, in order to apply this equation, one should have knowledge of velocity field beforehand. This is one of the limitations of application of Bernoulli’s equation.

Irrotationality of flow field

Under some special condition, the constant C becomes invariant from streamline to streamline and the Bernoulli’s equation is applicable with same value of C to the entire flow field. The typical condition is the irrotationality of flow field.

Proof:

Let us consider a steady two dimensional flow of an ideal fluid in a rectangular Cartesian coordinate system. The velocity field is given by

hence the condition of irrotationality is

The steady state Euler’s equation can be written as

We consider the y-axis to be vertical and directed positive upward. From the condition of irrotationality given by the Eq. (14.1), we substitute in place of in the Eq. 14.2a and in place of in the Eq. 14.2b. This results in

Now multiplying Eq.(14.3a) by ‘dx’ and Eq.(14.3b) by ‘dy’ and then adding these two equations we have

The Eq. (14.4) can be physically interpreted as the equation of conservation of energy for an arbitrary displacement

. Since, u, v and p are functions of x and y, we can write

With the help of Eqs (14.5a), (14.5b), and (14.5c), the Eq. (14.4) can be written as

The integration of Eq. 14.6 results in

For an incompressible flow,

The constant C in Eqs (14.7a) and (14.7b) has the same value in the entire flow field, since no restriction was made in the choice of dr which was considered as an arbitrary displacement in evaluating the work.

Note: In deriving Eq. (13.8) the displacement ds was considered along a streamline. Therefore, the total mechanical energy remains constant everywhere in an inviscid and irrotational flow, while it is constant only along a streamline for an inviscid but rotational flow.

The equation of motion for the ﬂow of an inviscid fluid can be written in a vector form as