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Fluid mechanics properties

FLUID PROPERTIES 

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Define fluid. 
A Fluid is a substance that deforms continuously when subjected to a shear stress no matter how small that shear stress may be.

Differentiate solid and fluid. 
Fluid
The fluid deforms continuously when subjected to a shear stress.
When the shear stress disappears the fluid never regain in to original shape. .
Solid

The Solid deforms a definite amount when subjected to a shear stress
When the shear stress disappears solids gain fully or partly their original shape.

Define density. 
Density is defined as the mass of a substance per unit volume.
If a fluid element enclosing a point P has a volume dV and dm , then the density is given by r = lim dV - 0 (dm / dV) = (dm / dV) The unit of density is kg/m3 .

Define specific volume,. 
Specific volume is defined as the reciprocal of density that is volume capacity per unit mass of fluid
Vs = ( 1 / r) = ( dV / dm ) The unit of sp. Volume is m3/kg

Define specific weight. 
Specific weight is the weight of the fluid per unit volume.
g = ( weight / volume) = ( m g / v) = r g The unit of specific weight is N/m3.

Define specific gravity (SG). 
Specific gravity is the ratio of mass density (or) weight density of the fluid to the mass density (or) weight density of the standard fluid. For liquids, water at 4oc is considered as standard fluid.
A liquid has a specific gravity of 1.527

what are the values of specific weight and specific volume ?
Specific gravity of a liquid (SG) = Sp. Weight (or) weight density of liquid / Sp. Weight (or) weight density of std liquid The standard liquid is water and its specific weight = r g = 1000 x 9.81 = 9810 N/m3
The specific weight of the liquid = 9810 x 1.527 = 14979.8 N/m3.
Density of the liquid ( r ) = 14979.8 / 9.81 = 1527 kg/ m3.
Specific volume of liquid = 1 /r = 1 / 1527 = 6.54 x 10 –4 m3/kg.

Define viscosity. 
The viscosity can be defined as the property of fluid which resist relative motion of its adjacent layers. It is the measure of internal fluid friction due to which there is resistance to flow, The unit of viscosity is Ns/m2.

State Newton’s law of viscosity. (AU-MQP)
The shear stress on a fluid element layer is directly proportional to the rate of strain (or) velocity gradient, the constant of proportionality being called the coefficient of viscosity.
t a (du / dy) shear stress ( t ) = m (du / dy)

what is real fluid ? Give examples. (AU-M03). 
The fluids in reality have viscosity m > 0 hence they are termed as real fluids and their motion is known as viscous flow. (ex) Air , water, kerosene, blood, milk

Why are some fluids are classified as Newtonian fluid ? Give examples of Newtonian fluids. (AU-N02).
The fluids, which obey Newton’s law of viscosity are known as Newtonian fluids. For these fluids, there is a linear relationship between shear stress and velocity gradient. (ex) Air, water, kerosene.

What is a Tthyxotropic fluid ? (AU- N 03)
If the viscosity increases with time the fluid is said to be a Thyxotropic fluid. (ex) Lipstick, paints enamels, crude oil.

What is a Rheopectic fluid ? 
If the viscosity decreases with time the fluid is said to be Rheopectic fluid. (ex) gypsum suspension, bentonite clay solution.

What is effect of temperature on viscosity of water and air ? 
*The viscosity of water decreases with increase in temperature.
*The viscosity of air increases with increase in temperature.

Define kinematic viscosity and gives its uint. 
Kinematic viscosity is defined as the ratio of dynamic viscosity to density.
n = m / r The unit of kinematic viscosity is m2/s

What is compressibility of fluid ? 
Compressibility of substance is the measure of its change in volume under the action of external forces, namely, the normal compressive forces. The measure of compressibility of the fluid is the bulk modulus of elasticity (K)
K = lim DV - 0 (- DP) / (DV/V) The unit of compressibility is N/m2

Assuming the bulk modulus of elasticity of water is 2.07 x 106 kN/m2 at standard atmospheric condition. Determine the increase of pressure necessary to produce one percent reduction in volume at same temperature. (AU-N02)
Bulk modulus of elasticity K = 2.07 x 106 kN/m2 - (dV/V) = 1% = 0.01
K = - dP / (dV/V) \ Increase in pressure dP = -(dV/V) x K
= 0.01 x 2.07 x 106 = 20700 kN/m2.

What is meant by vapor pressure of a liquid ? 
Liquids evaporate because of molecule s escaping from the liquid surface. These vapor molecules exert a partial pressure on the surface of the liquid known as vapour pressure.

What is cavitation ? 
In flowing fluid, if the pressure is equal to or less than the saturated vapor pressure, the liquid boil locally and produce vapor bubbles. These bubbles collapse in the high pressure region causing a partial vaccum. This phenomenon in known as cavitation.

Define surface tension and mention its unit. 
A free surface of the liquid is always under stretched condition implying the existence of tensile force on the surface. The magnitude of this force per unit length of an imaginary line drawn along the liquid surface is known as surface tension. The unit of surface tension is N/m.

Define capillarity. (AU-M04) 
Capillary implies the raise or depression of liquid in a capillary tube where it is held vertically or inclined in the liquid.

Define the pressure and mention its unit. 
If the fluid is stationary, then the force (dF) exerted by the fluid on the area is normal to the surface (dA). This normal force per unit area is called pressure..
P = ( dF / dA) The unit of pressure is N/m2.

What should be the depth of oil of specific gravity 0.8, if it has exerted a pressure of 480N/m2 ? 
Specific gravity (SG) = 0.8 \ density = 800 kg/m3
The pressure = r g z depth z = P/(r g) = 480 x 103 / (800 x 9.81) = 61.16 m
Express 3m of water head in cm of mercury.
rm gm Hm = rw gw Hw 13600 x Hm = 1000 x 3 Hm = 0.22 m of Hg

Differentiate between absolute and gauge pressure. 
Absolute pressure is measured as a pressure above absolute zero
Gauge pressure is measured as a pressure below atmospheric pressure
Gauge pressure = Absolute pressure - Atmospheric pressure

What do you mean by vacuum pressure ? 
If the pressure is less than the local atmospheric pressure it is called as vacuum pressure.
Vacuum pressure = Atmospheric pressure - Absolute pressure

What is a manometer ? Name the common fluids used in it. 
A manometer is a transparent tube containing a liquid of known density used for the purpose of measuring the fluid pressure. The common fluids used are mercury, alcohol.

Differentiate between simple manometer and differential manometer. 
Simple manometer
In simple manometer, one end is connected to the point at which the pressure is to be measured and the other end is open to atmosphere.

Differential manometer
In differential manometer, two ends are connected to the points whose ‘difference of pressure’ is to be measured.

What is micro-manometer ? Where is it used ? 
In this manometer a large difference in meniscus levels are obtained for very small pressure difference. This manometer is useful for precise measurement of pressure difference.

Design for Static and Dynamic Loading

Design for Static and Dynamic Loading

Machine parts fail when the stresses induced by external forces exceed their strength. The external loads cause internal stresses in the elements and the component size depends on the stresses developed.

Loading may be due to:

• The energy transmitted by a machine element.
• Dead weight.
• Inertial forces.
• Thermal loading.
• Frictional forces.

Load may be classified as:

• Static load- Load does not change in magnitude and direction and normally increases gradually to a steady value.

• Dynamic load- Load may change in magnitude for example, traffic of varying weight passing a bridge. Load may change in direction, for example, load on piston rod of a double acting cylinder. Vibration and shock are types of dynamic loading.

Avogadro’s number

Avogadro’s number

A mole is simply Avogadro's number of things. In chemistry, those "things" are atoms or molecules. In theory, you could have a mole of baseballs or anything else, but given that a mole of baseballs would cover the Earth to a height of several hundred miles, you'd be hard-pressed to find good practical use for a mole of anything bigger than a molecule [source: Hill and Kolb]. So if the mole is only used for chemistry, how did Amedeo Avogadro and chemistry cross paths  Born in Italy in 1776, Avogadro grew up during an important period in the development of chemistry. Chemists like John Dalton and Joseph Louis Gay-Lussac were beginning to understand the basic properties of atoms and molecules, and they hotly debated how these infinitesimally small particles behaved. Gay-Lussac's law of combining volumes particularly interested Avogadro. The law stated that when two volumes of gases react with one another to create a third gas, the ratio between the volume of the reactants and the volume of the product is always made of simple whole numbers. Here's an example: Two volumes of hydrogen gas combine with one volume of oxygen gas to form two volumes of water vapor (at least when temperatures are high enough) with nothing left over, or:

2H2 + O2 --> 2H2O

Tinkering around with the implications of this law, Avogadro deduced that in order for this to be true, equal volumes of any two gases at the same temperature and pressure must hold an equal number of particles (Avogadro's law). And the only way to explain that this law could be true for any example, including the one we just mentioned, is if there was a difference between atoms and molecules and that some elements, like oxygen, actually exist as molecules (in oxygen’s case, O2 rather than simply O) Granted, Avogadro didn't have words like "molecule" to describe his theory, and his ideas met resistance from John Dalton, among others. It would take another chemist by the name of Stanislao Cannizzaro to bring Avogadro's ideas the attention they deserved. By the time those ideas gained traction, the Italian with the crazy long name had already passed away.

So where does Avogadro's number fit into this? Because Avogadro's law proved so critical to the advancement of chemistry, chemist Jean Baptiste Perrin named the number in his honor. Read on to see how chemists determined Avogadro's number and why, even today, it's such an important part of chemistry.

Area Formulas

Area Formulas

Square = a ² 
Rectangle = ab 
Parallelogram = bh 
Trapezoid = h/2 (b₁ + b₂) 
Circle = pi r ² 
Ellipse = pi r₁ r₂ 

triangle =

one half times the base length times the height of the triangle

  

equilateral triangle =

triangle given SAS (two sides and the opposite angle)= (1/2) a b sin C

triangle given a,b,c = [s(s-a)(s-b)(s-c)] when s = (a+b+c)/2 (Heron's formula)

regular polygon = (1/2) n sin(360°/n) S²
   when n = # of sides and S = length from center to a corner

   Units

Area is measured in "square" units. The area of a figure is the number of squares required to cover it completely, like tiles on a floor.

Area of a square = side times side. Since each side of a square is the same, it can simply be the length of one side squared.

If a square has one side of 4 inches, the area would be 4 inches times 4 inches, or 16 square inches. (Square inches can also be written in².)

Be sure to use the same units for all measurements. You cannot multiply feet times inches, it doesn't make a square measurement.

Volume Formulas

Volume Formulas

cube = a ³ 

rectangular prism = a b c 

irregular prism = b h 

cylinder = b h = pi r ² h 

pyramid = (1/3) b h 

cone = (1/3) b h = 1/3 pi r ² h 

sphere = (4/3) pi r ³ 

ellipsoid = (4/3) pi r₁ r₂ r₃ 

Units

Volume is measured in "cubic" units. The volume of a figure is the number of cubes required to fill it completely, like blocks in a box.

Volume of a cube = side times side times side. Since each side of a square is the same, it can simply be the length of one side cubed.

If a square has one side of 4 inches, the volume would be 4 inches times 4 inches times 4 inches, or 64 cubic inches. (Cubic inches can also be written in³.)

Be sure to use the same units for all measurements. You cannot multiply feet times inches times yards, it doesn't make a perfectly cubed measurement.

Fluid Mechanics - Law of Continuity

 Law of Continuity

Any fluid moving through a pipe obeys the Law of Continuity, which states that the product of average velocity (v), pipe cross-sectional area (A), and fluid density (ρ) for a given flow stream must remain constant:

 

Fluid continuity is an expression of a more fundamental law of physics: the Conservation of Mass. If we assign appropriate units of measurement to the variables in the continuity equation, we see that the units cancel in such a way that only units of mass per unit time remain:

 

This means we may define the product ρAv as an expression of mass flow rate, or W:

In order for the product  to differ between any two points in a pipe, mass would have to mysteriously appear and disappear. So long as the flow is continuous (not pulsing), and the pipe does not leak, it is impossible to have different rates of mass flow at different points along the flow path without violating the Law of Mass Conservation. The continuity principle for fluid through a pipe is analogous to the principle of current being the same everywhere in a series circuit, and for equivalently the same reason₁.

We refer to a flowing fluid as incompressible if its density does not substantially change₂. For this limiting case, the continuity equation simplifies to the following form:

Examining this equation in light of dimensional analysis, we see that the product Av is also an expression of flow rate:

Cubic meters per second is an expression of volumetric flow rate, often symbolized by the variable Q:

 

The practical implication of this principle is that fluid velocity is inversely proportional to the cross-sectional area of a pipe. That is, fluid slows down when the pipe’s diameter expands, and visa-versa. We see this principle easily in nature: deep rivers run slow, while rapids are relatively shallow (and/or narrow).

For example, consider a pipe with an inside diameter of 8 inches (2/3 of a foot), passing a liquid flow of 5 cubic feet per minute. The average velocity (v) of this fluid may be calculated as follows:

 

Solving for A in units of square feet:

 

Now, solving for average velocity v:

 

 

₁In an electric circuit, the conservation law necessitating equal current at all points in a series circuit is the Law of Charge Conservation.

₂Although not grammatically correct, this is a common use of the word in discussions of fluid dynamics. By definition, something that is “incompressible” cannot be compressed, but that is not how we are using the term here. We commonly use the term “incompressible” to refer to either a moving liquid (in which case the actual compressibility of the liquid is inconsequential) or a gas/vapor that does not happen to undergo substantial compression or expansion as it flows through a pipe. In other words, an “incompressible” flow is a moving fluid whose ρ does not substantially change, whether by actual impossibility or by circumstance.

Kepler's Laws

Kepler's Laws

Johannes Kepler, working with data painstakingly collected by Tycho Brahe without the aid of a telescope, developed three laws which described the motion of the planets across the sky.

1. The Law of Orbits: All planets move in elliptical orbits, with the sun at one focus.

2. The Law of Areas: A line that connects a planet to the sun sweeps out equal areas in equal times.

3. The Law of Periods: The square of the period of any planet is proportional to the cube of the semimajor axis of its orbit.

Kepler's laws were derived for orbits around the sun, but they apply to satellite orbits as well.

The Law of Orbits

All planets move in elliptical orbits, with the sun at one focus.

This is one of Kepler's laws. The elliptical shape of the orbit is a result of the inverse square force of gravity. The eccentricity of the ellipse is greatly exaggerated here

Orbit Eccentricity The eccentricity of an ellipse can be defined as the ratio of the distance between the foci to the major axis of the ellipse. The eccentricity is zero for a circle. Of the planetary orbits, only Pluto has a large eccentricity. Examples of Ellipse Eccentricity Planetary orbit eccentricities Mercury .206 Venus .0068 Earth .0167 Mars .0934 Jupiter .0485 Saturn .0556 Uranus .0472 Neptune .0086 Pluto .25 The Law of Areas A line that connects a planet to the sun sweeps out equal areas in equal times. This is one of Kepler's laws.This empirical law discovered by Kepler arises fromconservation of angular momentum. When the planet is closer to the sun, it moves faster, sweeping through a longer path in a given time.

The Law of Periods

The square of the period of any planet is proportional to the cube of the semimajor axis of its orbit.

This is one of Kepler's laws.This law arises from the law of gravitation. Newton first formulated the law of gravitation from Kepler's 3rd law.

Kepler's Law of Periods in the above form is an approximation that serves well for the orbits of the planets because the Sun's mass is so dominant. But more precisely the law should be written

In this more rigorous form it is useful for calculation of the orbital period of moons or other binary orbits like those of binary stars.

Data: Law of Periods

Data confirming Kepler's Law of Periods comes from measurements of the motion of the planets.

Planet	Semimajor axis (1010m)	Period T (y)	T2/a3 (10-34y2/m3)
Mercury	5.79	0.241	2.99
Venus	10.8	0.615	3.00
Earth	15.0	1	2.96
Mars	22.8	1.88	2.98
Jupiter	77.8	11.9	3.01
Saturn	143	29.5	2.98
Uranus	287	84	2.98
Neptune	450	165	2.99
Pluto	590	248	2.99

The quantity T²/a³ depends upon the sum of the masses of the Sun and the planet, but since the mass of the Sun is so great, adding the mass of the planet makes very little difference.

Data from Halliday, Resnick, Walker, Fundamentals of Physics 4th Ed Extended.

Intercooler

Intercooler

An intercooler is an intake air cooling device commonly used on turbocharged and supercharged engines.

An intercooler cools the air compressed by the turbo/supercharger, reducing its temperature and thereby increasing the density of the air supplied to the engine.

As the air is compressed by a turbo/supercharger it gets very hot, very quickly. As its temperature climbs, its oxygen content (density) drops, so by cooling the air, an intercooler allows denser, more oxygen rich air to the engine, allowing more fuel to be burned, thus improving combustion and giving more power. It also increases reliability as it provides a more consistent temperature of intake air to the engine which allows the air fuel ratio of the engine to remain at a safe and steady level.

There are two types of intercoolers; Air-to-Air and Air-to-Water.

An Air-to-Air intercooler extracts heat from the compressed air by passing it through its network of tubes with cooling fins. As the compressed air is pushed through the intercooler it transfers the heat to the tubes and, in turn to the cooling fins. The cool air from outside, traveling at speed, absorbs the heat from the cooling fins reducing the temperature of the compressed air. The advantages of this system are simplicity, lower cost and light weight. These factors make it by far the most common form of intercooling. The down sides can be a longer intake length (as the intercooler is usually at the front of the car) and more variation in temperature than the Air-to-Water type.

An Air-to-Water intercooler uses water as a heat transfer agent. In this setup cool water is pumped through the air/water intercooler, extracting heat from the compressed air as it passes through. The heated water is then pumped through another cooling circuit (usually a dedicated radiator) while the cooled compressed air is pushed into the engine.

These intercoolers (also known as heat exchangers) tend to be smaller than their Air-to-Air counterparts making them well suited to difficult installations where space, airflow and intake length are an issue. Water is more efficient at heat transfer than air and has more stability so it can handle a wider range of temperatures.

On the downside the Air-to-Water system is complex, heavy and has the added cost of a radiator, a pump, water and transfer lines. Common applications for these are industrial machinery, marine and custom installs that don’t allow the easy fitment of an air to air intercooler, such as a rear-engined vehicle.

Intercooler placementThe best placement for an air to air is in the at the front of the vehicle. The “front-mount” is considered to be the most effective placement.

When the engine layout, or type of the vehicle do not permit the “front-mount” placement, an intercooler can be mounted on top of the engine, or even on its side, but these are not considered as effective as the air flow is not as good and the intercooler can suffer from heat soak from the engine when the external airflow drops. These placements will often require additional air ducts or scoops to route the air directly into the intercooler.

Subaru’s trademark top-mount requires a scoop in the bonnet to route the airflow onto the intercooler.

The Air-to-Water system can be mounted anywhere in the engine bay, as long as the radiator is mounted in a position where it receives good airflow, and/or with a thermo fan attached to it.