Lecture on Bernoulli's Equation
Introduction
- Fundamental aerodynamic equation: Bernoulli's equation
- Used to calculate pressures and velocities in incompressible flows.
Background
- Derived from the Euler equation for fluid flow based on Newton's second law (force = mass x acceleration).
- Euler equation:
dp = -rhoVdV
- Assumptions: Steady flow, no gravity, no viscosity forces.
Derivation of Bernoulli's Equation
- Integrate Euler equation along a streamline between two points (1 and 2):
- Integral of
dp
from p1
to p2
plus integral from v1
to v2
of rhoVdV = 0
.
- Develops into:
p2 - p1 + rho(1/2 V2^2 - 1/2 V1^2) = 0
.
- Rearranged:
p1 + 1/2 rhoV1^2 = p2 + 1/2 rhoV2^2
.
- Along a streamline:
p + 1/2 rhoV^2 = constant
.
- Terminology:
- Total Pressure (pt): Constant along streamline.
- Static Pressure (p): Pressure at a point.
- Dynamic Pressure (1/2 rho V^2).
- Known as Bernoulli's principle or Bernoulli's equation.
Historical Context
-
Daniel Bernoulli:
- Born in January 1700, Groningen, Netherlands.
- Family from Basel, Switzerland, moved back when Daniel was 5.
- Influenced by father Johann Bernoulli, a renowned mathematician.
- Initially studied philosophy, logic, and medicine.
- Academic career: Chair of mathematics at University of St. Petersburg.
-
Significant Works:
- Published Hydrodynamica in 1738, basis for Bernoulli’s equation.
- Relationship with Euler who contributed to the derivation.
- Awarded prestigious Prize of the Paris Academy of Sciences 10 times.
Practical Applications
Conclusion
- Bernoulli's equation applicable in incompressible flows, neglecting viscosity.
- Next lecture will explore compressible flows.
Note: These points provide a high-level summary and reference to the key concepts and historical context presented in the lecture on Bernoulli's equation, including its derivation, historical significance, and practical applications.