Viscous Flow Flashcards
What is viscosity?
What are the 2 types?
The MEASURE of RESISTANCE to the RELATIVE MOVEMENT between TWO NEIGHBOURING PARTICLES of a fluid; DYNAMIC viscosity (μ): A MEASURE of INTERNAL RESISTANCE on the TANGENTIAL FORCE per unit REQUIRED to MOVE HORIZONTAL PLANE with respect to another at a unit VELOCITY while maintaining a unit DISTANCE APART (Pa.s); KINEMATIC viscosity (ν): The RATIO of DYNAMIC viscosity to DENSITY ν = μ/ρ (m^2/s)
What is viscous shear stress?
What is the equation?
What does each component represent?
The FORCE due to the INTERACTION BETWEEN fluid PARTICLES, PROPORTIONAL to the VELOCITY CHANGE in the DIRECTION PERPENDICULAR to VELOCITY;
τ = μ(∂u/∂y);
μ: DYNAMIC VISCOSITY of the the fluid;
u: VELOCITY of the FLUID particle along its STREAMLINE;
y: DIRECTION PERPENDICULAR to u
What is the effect of increasing temperature on viscosity?
Normally, VISCOSITY of LIQUID DECREASES as the BONDS between molecules become more RELAXED, and the MOLECULES are LESS RESTRICTED;
VISCOSITY of GASES will INCREASE as the INTERNAL ENERGY INCREASES so the MOLECULES move FASTER and COLLISIONS occur more FREQUENTLY causing more RESISTANCE of the CHANGE of RELATIVE VELOCITY
What is the effect of increasing pressure on viscosity?
INCREASING PRESSURE will INCREASE VISCOSITY of LIQUID and GAS as the MOLECULES are COMPRESSED CLOSER together, INCREASING SHEAR STRESS;
However, for a LIQUID to CHANGE VISCOSITY, SIGNIFICANT PRESSURE must be APPLIED as they often have LITTLE to NO COMPRESSIBILITY
Explain why Bernoulli’s equation must be changed when considering a viscous fluid?
When a VISCOUS fluid travels from A to B ENERGY is CONSUMED to OVERCOME the FRICTION BETWEEN fluid PARTICLES and BETWEEN FLUID and the SURFACE;
This means H will be LESS at B and PRESSURE will be LOST so hf is added to the equation to ACCOUNT for LOSS of PRESSURE HEAD along the STREAMLINE
What is Reynolds number?
What is the equation?
What does each component represent?
A DIMENSIONLESS number which is used to CHARACTERISE the REGIME of a FLOW by showing the RATIO of INERTIAL FORCE of the FLUID to FRICTION due to VISCOSITY of fluid; Re = ρvL/μ or Re = vL/ν; ρ: DENSITY of fluid (kg/m^3); v: MEAN VELOCITY of fluid (m/s); L: CHARACTERISTIC LENGTH of fluid (m); μ: DYNAMIC VISCOSITY of fluid (Pa.s); ν: KINEMATIC VISCOSITY of fluid (m^2/s)
What are the two regimes of fluid flow?
Give a brief description of each?
LAMINAR flow: Fluid PARTICLES move in ORDERLY LAYERS;
TURBULENT flow: Fluid PARTICLES may ROTATE, COLLIDE with each other and move RANDOMLY in DIFFERENT DIRECTIONS
For internal pipe flow, what are the Re values that determine the regime of the flow?
LAMINAR: Re < 2000
TURBULENT: Re > 4000
TRANSITION: 2000 < Re < 4000
Explain the main characteristics of the structure of the boundary layer on an aerofoil?
The boundary layer is a LAYER of FLUID in the PROXIMITY of a SURFACE where the EFFECTS of VISCOSITY are SIGNIFICANT;
At the SURFACE the SPEED is 0m/s and INCREASES with DISTANCE PERPENDICULAR to the SURFACE until reaching the SPEED of the MAIN FLOW;
The THICKNESS is determined by the DISTANCE between the SURFACE and the location where SPEED is 0.99 of the FULL LOCAL SPEED;
As air moves from LEADING EDGE it ENTERS LAMINAR BOUNDARY layer, which has a relatively THIN, UNIFORM FLOW and the SPEED INCREASES approximately LINEARLY PERPENDICULAR to the surface;
The air experiences a TRANSITION PERIOD in the INCREASING X DIRECTION from LAMINAR to TURBULENT known as the TRANSITION REGION;
The air then enters the TURBULENT BOUNDARY layer which has THICKER, more RANDOM flow and SPEED INCREASES STEEPLY close to the SURFACE then becomes UNIFORM near the EDGE of the BOUNDARY layer;
The TURBULENT layer also has a VISCOUS LAMINAR SUB-LAYER just over the SURFACE and BUFFER ZONE between the TRANSITION from LAMINAR SUB-LAYER to main TURBULENT BOUNDARY layer
How does pressure change within the boundary layer?
PRESSURE remains CONSTANT in PERPENDICULAR DIRECTION to the surface;
PRESSURE will CHANGE with the PRESSURE OUTSIDE the BOUNDARY LAYER in the PARALLEL DIRECTION to the surface;
According to BERNOULLI’S and the CONTINUITY equation, at the LEADING EDGE the FLOW path gets NARROWER causing PRESSURE to DECREASE and as the air flows OVER the MOST CAMBERED POINT the air PRESSURE INCREASES
How does velocity change within the boundary layer?*****
In LAMINAR boundary layer SPEED INCREASES approximately LINEARLY in the DIRECTION PERPENDICULAR to the SURFACE;
In TURBULENT boundary layer SPEED INCREASES SIGNIFICANTLY/EXPONENTIALLY in the DIRECTION PERPENDICULAR to the SURFACE when it is very CLOSE to the SURFACE then the INCREASE SLOWS as the VERTICAL DISTANCE from the surface INCREASES
For flow over a flat plate, what are values determine the regime of the flow?
LAMINAR: Re < 5x10^5
TURBULENT: Re > 5x10^6
TRANSITION: 5x10^5 < Re < 5x10^6
How does viscous shear stress relate to skin drag?
There is SHEAR STRESS in the BOUNDARY LAYER due to the CHANGE in VELOCITY PERPENDICULAR to the surface which ACTS PARALLEL to the surface;
When this SHEAR STRESS occurs the INTEGRATION of it provides SKIN DRAG therefore the HIGHER the VISCOUS SHEAR STRESS the GREATER the SKIN DRAG
Compare the speed profiles of the laminar and turbulent boundary layers NEAR THE SURFACE?
The TURBULENT SPEED PROFILE graph is much FLATTER than the LAMINAR over the THICKNESS of the BOUNDARY LAYER;
This means the AVERAGE SPEED of the TURBULENT layer is GREATER and therefore the PARTICLES have MORE KINETIC ENERGY;
Because of the GREATER CHANGE in VELOCITY in the Y DIRECTIONS, SHEAR STRESS is GREATER in TURBULENT layer τ = μ(∂u/∂y) meaning the SKIN DRAG will also be GREATER
What happens to the size of the boundary layer as the distance increases from the leading edge? Why?
In VISCOUS flow, fluid must CONSUME KINETIC ENERGY to OVERCOME the RESISTANCE caused by VISCOSITY;
The LONGER the fluid TRAVELS along the SURFACE, the MORE KINETIC ENERGY will be LOST and the MORE VERTICAL DISTANCE is required to INCREASE the SPEED to MAIN STREAM;
This means the BOUNDARY LAYER will LOSE MORE MOMENTUM, and get THICKER and THICKER along the surface