The Physics Hypertextbook™
© 1998-2008 by Glenn Elert -- A Work in Progress
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All things are flowing -- Heraclitus ca. 500 BCE
When a fluid flows is an incompressible manner …
| φ = | V | = Av = constant | ⇒ | A1v1 = A2v2 |
| t |
If the fluid is compressible, then …
| I = | m | = ρAv = constant | ⇒ | ρ1A1v1 = ρ2A2v2 |
| t |
Bernoulli's equation is based on the law of conservation of energy; the increased kinetic energy of a fluid is offset by a reduction of the "static energy" associated with pressure. The fluid is assumed incompressible and inviscid (that is, the fluid does not generate drag).
Something like this is right, but this derivation must certainly be wrong. (It has a glaring algebra error. Can you spot it?)
| W | = | ΔE | ||||
| PΔV | = | ΔU | + | ΔK | ||
| P2V2 | − | P1V1 | = | U2 − U1 | + | K2 − K1 |
Rearrange
| P1V1 | + | U1 | + | K1 | = | P2V2 | + | U2 | + | K2 |
| P1V1 | + | mgh1 | + | ½ mv12 | = | P2V2 | + | mgh2 | + | ½ mv12 |
| P1V1 | + | mgh1 | + | ½ mv12 | = | P2V2 | + | mgh2 | + | ½ mv12 |
| V1 | V1 | V1 | V2 | V2 | V2 | |||||
| P1 | + | ρgh1 | + | ½ ρv12 | = | P2 | + | ρgh2 | + | ½ ρv12 |
The conclusion is right
P1 + ρgh1 + ½ ρv12 = P2 + ρgh2 + ½ ρv12
The third term in this equation is the dynamic pressure (q).
q = ½ ρv12
The space shuttle and "Max. Q".
| Δm | = | ρΔV | = | ρAΔs | = ρAv = constant |
| Δt | Δt | Δt | |||
| P1 + ½ ρv12 + ρgh1 = P2 + ½ ρv22 + ρgh2 |
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