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Bernoulli's Theorem

In its most general form, Bernoulli's theorem--which was discovered by Daniel Bernoulli (1700-1783)--states that, in the steady flow of an inviscid fluid, the quantity
\frac{p}{\rho} + {\cal T}
\end{displaymath} (432)

is constant along a streamline, where $p$ is the pressure, $\rho$ the density, and ${\cal T}$ the total energy per unit mass.

Figure 20: Bernoulli's theorem.
\epsfysize =2.75in

The proof is straightforward. Consider the body of fluid bounded by the cross-sectional areas $AB$ and $CD$ of the stream filament pictured in Figure 20. Let us denote the values of quantities at $AB$ and $CD$ by the suffixes $1$ and $2$, respectively. Thus, $p_1$, $v_1$, $\rho_1$, $S_1$, ${\cal T}_1$ are the pressure, fluid speed, density, cross-sectional area, and total energy per unit mass, respectively, at $AB$, etc. Suppose that, after a short time interval $\delta t$, the body of fluid has moved such that it occupies the section of the filament bounded by the cross-sections $A'B'$ and $C'D'$, where $AA'=v_1\,\delta t$ and $CC'=v_2\,\delta t$. Since the motion is steady, the mass $m$ of the fluid between $AB$ and $A'B'$ is the same as that between $CD$ and $C'D'$, so that

m= S_1\,v_1\,\delta t\,\rho_1=S_2\,v_2\,\delta t\,\rho_2.
\end{displaymath} (433)

Let $T$ denote the total energy of the section of the fluid lying between $A'B'$ and $CD$. Thus, the increase in energy of the fluid body in the time interval $\delta t$ is
(m\,{\cal T}_2+T)-(m\,{\cal T}_1+T)=m\,({\cal T}_2-{\cal T}_1).
\end{displaymath} (434)

In the absence of viscous energy dissipation, this energy increase must equal the net work done by the fluid pressures at $AB$ and $CD$, which is
p_1\,S_1\,v_1\,\delta t - p_2\,S_2\,v_2\,\delta t = m\left(\frac{p_1}{\rho_1}-\frac{p_2}{\rho_2}\right).
\end{displaymath} (435)

Equating expressions (434) and (435), we find that
\frac{p_1}{\rho_1}+ {\cal T}_1= \frac{p_2}{\rho_2}+{\cal T}_2,
\end{displaymath} (436)

which demonstrates that $p/\rho+{\cal T}$ has the same value at any two points on a given stream filament, and is therefore constant along the filament. Note that Bernoulli's theorem has only been proved for the case of the steady motion of an inviscid fluid. However, the fluid in question may either be compressible or incompressible.

For the particular case of an incompressible fluid, moving in a conservative force-field, the total energy per unit mass is the sum of the kinetic energy per unit mass, $(1/2)\,v^2$, and the potential energy per unit mass, ${\mit\Psi}$, and Bernoulli's theorem thus becomes

\frac{p}{\rho} + \frac{1}{2}\,v^2 + {\mit\Psi} = \mbox{constant along a streamline}.
\end{displaymath} (437)

If we focus on a particular streamline, 1 (say), then Bernoulli's theorem states that
\frac{p}{\rho} + \frac{1}{2}\,v^2 + {\mit\Psi} = C_1,
\end{displaymath} (438)

where $C_1$ is a constant characterizing that streamline. If we consider a second streamline, 2 (say), then
\frac{p}{\rho} + \frac{1}{2}\,v^2 + {\mit\Psi} = C_2,
\end{displaymath} (439)

where $C_2$ is another constant. It is not generally the case that $C_1=C_2$. If, however, the fluid motion is irrotational then the constant in Bernoulli's theorem is the same for all streamlines (see Section 5.7), so that
\frac{p}{\rho} + \frac{1}{2}\,v^2 + {\mit\Psi} = C
\end{displaymath} (440)

throughout the fluid.

next up previous
Next: Vortex Lines, Vortex Tubes, Up: Incompressible Inviscid Fluid Dynamics Previous: Streamlines, Stream Tubes, and
Richard Fitzpatrick 2012-04-27