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Basics of Fluid Mechanics, 2014a

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10.1. INTRODUCTION 331<br />

The partial derivative <strong>of</strong> any vector, Υ, with respect to time is the same direction as<br />

the unit vector. Hence, the product <strong>of</strong> multiplication <strong>of</strong> the partial derivative with an<br />

unit vector is<br />

∂Υ ̂(Υ )<br />

∂l · = ∂Υ<br />

(10.27)<br />

Υ ∂l<br />

where Υ is any vector and Υ its magnitude. The right hand side <strong>of</strong> equation (10.26)<br />

U × Ω is perpendicular to both vectors U and Ω. Hence, the dot product <strong>of</strong> vector U<br />

with a vector perpendicular to itself must be zero. Thus equation (10.26) becomes<br />

or<br />

U ·∇<br />

{}}{<br />

U<br />

(<br />

∂U<br />

∂t + d U 2 ∫ ( dP<br />

dl 2 + g l + ρ<br />

) ) =<br />

(<br />

∂U<br />

∂t + d U 2 ∫ ( dP<br />

dl 2 + g l + ρ<br />

=0<br />

{ }} {<br />

U<br />

U · U × Ω (10.28)<br />

) ) =0 (10.29)<br />

The first time derivative <strong>of</strong> equation (10.28) can be manipulated as it was done before<br />

to get into derivative as<br />

∂U<br />

∂t = d ∫ ∂U<br />

dl (10.30)<br />

dl ∂t<br />

Substituting into equation (10.28) writes<br />

(<br />

d ∂U<br />

dl ∂t + U 2 ∫ ( ) ) dP<br />

2 + g l + =0 (10.31)<br />

ρ<br />

The integration with respect or along stream line, “l” is a function <strong>of</strong> time (similar<br />

integration with respect x is a function <strong>of</strong> y.) and hence equation (10.28) becomes<br />

Bernoulli On A Streamline<br />

∂U<br />

∂t + U 2 ∫ ( ) dP<br />

2 + g l + = f(t)<br />

ρ<br />

(10.32)<br />

In these derivations two cases where analyzed the first case, for irrotational<br />

Bernoulli’s equation is applied any where in the flow field. This requirement means<br />

that the flow field must obey U × Υ. The second requirement regardless whether the<br />

flow is irrotational or not, must be along a streamline where the value is only function <strong>of</strong><br />

the time and not location. The confusion transpires because these two cases are referred<br />

as the Bernoulli equation while they refer to two different conditions or situations 1 .For<br />

both Bernoulli equations the viscosity must be zero.<br />

1 It is interesting to point out that these equations where developed by Euler but credited to the last<br />

D. Bernoulli. A discussion on this point can be found in Hunter’s book at Rouse, Hunter, and Simon<br />

Ince. History <strong>of</strong> hydraulics. Vol. 214. Ann Arbor, MI: Iowa Institute <strong>of</strong> Hydraulic Research, State<br />

University <strong>of</strong> Iowa, 1957.

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