19.9
Flujo laminar constante en tubos circulares
El flujo de Hagen-Poiseuille describe el flujo constante e incompresible de un fluido viscoso a través de un tubo cilíndrico con un radio constante R.…
Considere el flujo constante e incompresible a través de un tubo cilíndrico recto de radio constante R, conocido como flujo de Hagen-Poiseuille.
La geometría cilíndrica permite el uso de las coordenadas r, θ y z para mediciones radiales, angulares y axiales.
El fluido que fluye paralelo al eje del tubo tiene un componente de velocidad puramente axial y varía solo con la distancia radial.
Estas condiciones simplifican las ecuaciones de Navier-Stokes, revelando un perfil de velocidad parabólica que muestra que la velocidad es más alta en el centro y disminuye hacia las paredes, llegando a cero en el límite.
Esto demuestra el flujo laminar, donde las partículas de fluido se mueven suavemente en capas organizadas.
La integración de este perfil sobre la sección transversal del tubo da la ley de Poiseuille, que expresa el caudal Q como dependiente de la cuarta potencia del radio del tubo, la viscosidad del fluido y el gradiente de presión.
La velocidad media V, calculada a partir de Q, es la mitad de la velocidad máxima observada en el centro del tubo.
Esta distribución de velocidad confirma que el flujo es más alto en el centro y disminuye parabólicamente a cero en la pared.
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Q1: What is the parabolic velocity profile in Hagen-Poiseuille flow?
In Hagen-Poiseuille flow, the velocity profile is parabolic, with maximum velocity at the tube's center and decreasing to zero at the wall due to viscous drag. This parabolic distribution arises from solving the simplified Navier-Stokes equations under steady, incompressible flow conditions. The no-slip condition at the boundary ensures zero velocity at the tube wall, creating the characteristic smooth, layered velocity distribution.
Q2: How does Poiseuille's law relate tube radius to flow rate?
Poiseuille's law expresses volumetric flow rate Q as dependent on the fourth power of the tube's radius R, the pressure gradient, and fluid viscosity. This fourth-power relationship means even small increases in radius dramatically boost flow rate. The law demonstrates why narrow channels like capillaries have significantly restricted flow compared to larger tubes under identical pressure conditions.
Q3: What role do cylindrical coordinates play in analyzing Hagen-Poiseuille flow?
Cylindrical coordinates (r, θ, z) align naturally with the tube's geometry, representing radial, angular, and axial dimensions. This coordinate system simplifies the Navier-Stokes equations because the velocity varies only with radial distance r and points purely along the z-axis. The symmetry of cylindrical geometry eliminates angular velocity components, reducing complexity and revealing the parabolic velocity profile.
Q4: Why is the mean velocity exactly half the maximum velocity in laminar tube flow?
The mean velocity V equals half the maximum velocity at the tube center because of the parabolic velocity distribution. Integrating the parabolic profile across the tube's cross-section yields this precise relationship. This predictable ratio confirms the layered, organized nature of laminar flow and allows engineers to calculate average transport rates from maximum velocity measurements.
Q5: What is the no-slip condition and how does it affect laminar flow?
The no-slip condition requires fluid velocity to be zero at the tube wall due to friction between fluid and the solid boundary. This boundary constraint forces the velocity to decrease parabolically from the center to the wall. The no-slip condition is fundamental to laminar flow, ensuring fluid particles move in parallel layers without lateral mixing or turbulence.
Q6: How do the Navier-Stokes equations simplify for Hagen-Poiseuille flow?
For Hagen-Poiseuille flow, the Navier-Stokes equations simplify because velocity has only an axial component and varies solely with radial distance. Angular and radial velocity components vanish, eliminating multiple terms. This reduction transforms the full three-dimensional equations into a simpler form, yielding the parabolic velocity profile and enabling direct calculation of flow rate and pressure relationships.
Q7: Why is Hagen-Poiseuille flow considered a foundational example of laminar flow?
Hagen-Poiseuille flow demonstrates laminar flow principles in their simplest form: steady, incompressible flow through a constant-radius tube with organized, parallel fluid layers. The analytical solution provides exact velocity and flow rate relationships, making it ideal for teaching fluid mechanics fundamentals. Its applicability to narrow channels like capillaries illustrates how laminar flow governs transport in biological and industrial systems.