This document discusses fluids and Bernoulli's principle in physics. It defines ideal fluids as those with steady, incompressible, nonviscous, and irrotational flow. It presents the equation of continuity which states that the density times area times velocity is constant for a fluid. Bernoulli's principle states that as the flow speed of a fluid increases, the pressure decreases, which has various applications such as in aircraft wings and Venturi tubes.
Report on Types of fluid flow
fluid dynamics
Introduction
In physics, fluid flow has all kinds of aspects: steady or unsteady, compressible or incompressible, viscous or non-viscous, and rotational or irrotational to name a few. Some of these characteristics reflect properties of the liquid itself, and others focus on how the fluid is moving. Note that fluid flow can get very complex when it becomes turbulent. Physicists haven’t developed any elegant equations to describe turbulence because how turbulence works depends on the individual system whether you have water cascading through a pipe or air streaming out of a jet engine. Usually, you have to resort to computers to handle problems that involve fluid turbulence. Types of fluid flow:
Aerodynamic force
Cavitation
Compressible flow
Couette flow
Free molecular flow
Incompressible flow
Report on Types of fluid flow
fluid dynamics
Introduction
In physics, fluid flow has all kinds of aspects: steady or unsteady, compressible or incompressible, viscous or non-viscous, and rotational or irrotational to name a few. Some of these characteristics reflect properties of the liquid itself, and others focus on how the fluid is moving. Note that fluid flow can get very complex when it becomes turbulent. Physicists haven’t developed any elegant equations to describe turbulence because how turbulence works depends on the individual system whether you have water cascading through a pipe or air streaming out of a jet engine. Usually, you have to resort to computers to handle problems that involve fluid turbulence. Types of fluid flow:
Aerodynamic force
Cavitation
Compressible flow
Couette flow
Free molecular flow
Incompressible flow
FLUID DYNAMICS
Basic terms.
Ideal Fluid.
Equation of Continuity.
Bernoulli's Theorem.
Application of Bernoulli’s Theorem.
FLUID:
A fluid is a substance which can flows.
Such as liquids , gases and plasma.
Example: Water, air etc…
Fluid Dynamics:Study of fluid in motion.
Viscosity:
The frictional effect b/w different layers of a flowing fluid is the viscosity of the fluid.
Drag Force:
An object moving through a fluid experiences a retarding force called a drag force.
Fluid Flow:
Streamline /Laminar Flow:
Every particle of fluid during flow has constant velocity, pressure , density and having regularity.
Turbulent Flow:
The irregular and non-steady fluid flow is called turbulent flow.
Velocity , pressure , and density remain non – uniform.
IDEAL FLUID:
Properties of Ideal Fluid:
Fluid is non-viscous (Internal Friction is neglected).
Fluid is incompressible (i.e. Constant Density).
Flow is Steady (Laminar).
Flow is irrotational (i.e. No angular momentum)
EQUATION OF CONTINUITY:
Statement:“It states that the product of the area and the fluid speed at all points along a pipe is constant for an incompressible fluid.”
Derivation:
𝐦𝐚𝐬𝐬=𝐝𝐞𝐧𝐢𝐬𝐭𝐲×𝐯𝐨𝐥𝐮𝐦𝐞
∆𝑚_1=𝜌𝐴_1 〖∆𝑥〗_1
∵〖∆𝑥〗_1=𝑣_1×∆𝑡
∆𝑚_1=𝜌𝐴_1 𝑣_1×∆𝑡
Similarly
∆𝑚_2=𝜌𝐴_2 〖∆𝑥〗_2
∵〖∆𝑥〗_1=𝑣_1×∆𝑡
∆𝑚_2=𝜌𝐴_2 𝑣_2×∆𝑡
Because the fluid is incompressible and the flow is steady, then
∆𝑚_1=∆𝑚_2
𝜌𝐴_1 𝑣_1×∆𝑡=𝜌𝐴_2 𝑣_2×∆𝑡
𝐴_1 𝑣_1=𝐴_2 𝑣_2
So the product:
𝐴𝑣=𝑐𝑜𝑛𝑠𝑡𝑎𝑛𝑡
It has Dimensions:
𝐴×∆𝑥/∆𝑡=𝑉𝑜𝑙𝑢𝑚𝑒/𝑡𝑖𝑚𝑒
It is either called Volume Flux or Flow Rate
The speed of water spraying from the end of a garden hose increases as the size of the opening is decreased with the thumb.
Bernoulli’s Theorem:
It is simply a statement of Law of conservation of energy applied to liquid in motion.
This theorem states that:
“For the steady flow of an ideal fluid, the total energy (i.e., sum of pressure, potential energy & kinetic energy) per unit volume remains constant through the flow.”
𝑃+𝜌𝑔ℎ+1/2 𝜌𝑣^2=𝑐𝑜𝑛𝑠𝑡𝑎𝑛𝑡
Proof:
The force exerted on lower segment:
𝐹_1=𝑃_1 𝐴_1
The Work Done by force on this segment is:
𝑊_1=𝐹_1 〖∆𝑥〗_1
𝑊_1=𝑃_1 𝐴_1 〖∆𝑥〗_1
Similarly on the upper segment:
𝑊_2=−𝑃_2 𝐴_2 〖∆𝑥〗_2
This work done is negative because the it is against Fluid Fow
The Force 𝐹_1 moves the Liquid a distance 〖∆𝑥〗_1 & the liquid moves a distance 〖∆𝑥〗_2 against the Force 𝐹_2.
Therefore, the net work done on liquid is:
𝑊=𝑃_1 𝐴_1 〖∆𝑥〗_1−𝑃_2 𝐴_2 〖∆𝑥〗_2
𝑊=𝑃_1 (𝐴_1 〖∆𝑥〗_1)−𝑃_2 (𝐴_2 〖∆𝑥〗_2)
∵𝐴_1 〖∆𝑥〗_1=𝐴_2 〖∆𝑥〗_2=m/ρ
𝑊=(𝑃_1−𝑃_2 )V
Part of this Work is utilized by the fluid in changing its Kinetic Energy & a part is used in changing its Gravitational Potential Energy:
∆𝐾.𝐸=1/2 𝑚𝑣_2^2−1/2 𝑚𝑣_1^2
∆𝑃.𝐸=𝑚𝑔ℎ_2−𝑚𝑔ℎ_1
None of the Work Done on the liquid has been used to overcome the internal friction because the liquid is non-viscous.
According to Law of Conservation of Energy:
𝑊=∆𝐾.𝐸+∆𝑃.𝐸
(𝑃_1−𝑃_2 )V=1/2 𝑚𝑣_2^2−1/2 𝑚𝑣
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2. 2
Fluids in Motion
⇒ The motion of real fluids is very
complicated and is not yet fully
understood.
⇒ We will only discuss the motion of
ideal fluids.
Ideal Fluids
1) Steady Flow: the velocity of the moving
fluid at any fixed point does not change with
time (not turbulent)
Ideal Fluids
3. 3
Ideal Fluids
2) Incompressible Flow: the fluid is incompressible
(density is constant)
3) Nonviscous Flow: friction within the fluid can be
ignored
4) Irrotational Flow: a tiny test body placed within
the fluid will not rotate about an axis through its
own center of mass
The equation of continuity:
ρ1A1 v1 = ρ2A2 v2
⇒ the flow speed increases
when we decrease the cross-
sectional area
A1 v1 = A2v2 (if ρ constant)
Applications of Bernoulli’s Equation Applications of Bernoulli’s Equation
4. 4
Applications of Bernoulli’s Equation Applications of Bernoulli’s Equation
Applications of Bernoulli’s Equation Applications of Bernoulli’s Equation