Fluid Statics & Dynamics Flashcards

1
Q

Define Fluid

A

A fluid is any substance that flows freely because its particles are not rigidly attached to one another. Fluids have no repeating crystalline structure.

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2
Q

State and explain Pascal’s Principle.

A

Pascal’s principle states that pressure applied to a confined fluid is transmitted undiminished throughout the confining vessel or system. Fluid force acts equally, at right angles, to every portion of its container surface.

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3
Q

Define buoyancy

A

Buoyancy is defined as the tendency of a body to float or rise when submerged in a fluid. Archimedes’ principle states: “A body wholly or partially immersed in a fluid is buoyed up by a force equal to the weight of the displaced fluid.” If the density of the body is greater than the fluid it displaces, it sinks. If its density is less, it floats.

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4
Q

State and explain Archimedes’ Principle

A

Archimedes’ principle states: “A body wholly or partially immersed in a fluid is buoyed up by a force equal to the weight of the displaced fluid.”

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5
Q

Define and explain mass flow rate.

A

The mass flow rate equals the product of the density of the fluid, the cross-sectional area of flow, and average velocity of the fluid. If specific volume is used, mass flow rate is equal to the product of cross-sectional area and average velocity divided by the specific volume of the fluid.

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6
Q

Define and explain Volumetric Flow Rate

A

The volumetric flow rate of a fluid is defined as the volume of the fluid that passes a
reference point per unit time. The volumetric flow rate equals the product of the average velocity of the fluid and the cross-sectional area of flow.

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7
Q

How are Volumetric and Mass Flow Rates related?

A

The mass flow rate and the volumetric flow rate are related by the density or, specific volume, of the fluid.

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8
Q

What is viscosity? How does temperature impact viscosity?

A
  • Physically, the viscosity of a fluid is a measure of its resistance to flow when subjected to a shear stress.
  • For liquids, viscosity decreases with increasing temperature.
  • For gases, viscosity increases with increasing temperature.
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9
Q

Describe the two types of fluid flow and their velocity profiles.

A

The first type is known as laminar, streamline, or viscous flow. The significance of these terms is:

  • The fluid particles move in parallel layers where the layers of fluid move
    smoothly over adjacent layers without mixing between them.
  • The particles move in definite and observable paths or streamlines.
  • The flow is characteristic of viscous fluid or is one in which viscosity plays a significant part.

The second type of flow is known as turbulent flow. It is characterized by irregular motion of the fluid molecules. This velocity profile is flattened at the centerline. For
well-developed turbulent flow, the average velocity is only slightly less than the
centerline velocity.

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10
Q

Explain the continuity of fluid flow.

A

Continuity of fluid flow, or steady flow, occurs when the same mass flow exists everywhere in a pipe, meaning that the same quantity of fluid flows past any two reference points along the pipe in any given time. The continuity fluid flow
equation, when applied to fluid flow, is merely a statement of the continuity of fluid flow.

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11
Q

What is the Continuity Equation?

A
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12
Q

State the conditions where Bernoulli’s equation may be applied.

A

Bernoulli’s equation applies only when the flow of the fluid is treated as ideal, with no fluid friction.

Bernoulli’s equation results from the application of the general energy equation to a steady flow system in which:

  1. No heat is transferred to or from the fluid
  2. No work is done by or on the fluid
  3. No change occurs in the internal energy of the fluid.
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13
Q

Write and Explain Bernoulli’s equation in terms of the general energy equation.

A

PE1 + KE1 + P1V1 = PE2 + KE2 + P2V2

Where

PE = potential energy (ft lbf)

KE = kinetic energy (ft lbf)

P = pressure (lbf /ft2)

V = volume (ft3)

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14
Q

State and explain the Bernoulli Equation with higher detail energy terms.

A
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15
Q

What is the NRC version of the Bernoullie equation?

A
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16
Q

What is elevation head?

A

Elevation head (z) represents the potential
energy the fluid possesses due to its elevation
above a reference level. It is expressed by
the vertical distance, in feet, between the
reference level and the level of the fluid.

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17
Q

What is velocity head?

A

Velocity head - (Vav)2/ 2g - represents the kinetic energy the fluid possesses due to its velocity. It is the height, in feet, to which the flowing fluid would rise in a column if all of its kinetic energy were converted to potential energy.

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18
Q

What is pressure head?

A

Pressure head (Pυ) represents the PV energy the fluid possesses due to its pressure. It is expressed by the height, in feet, of a column of the fluid whose weight is equivalent to the pressure of the fluid. This pressure is the static pressure, which is the sum of gravity, applied forces, and atmospheric pressure.

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19
Q

Explain and distinguish between static pressure, dynamic pressure and total pressure.

A

Static pressure in a fluid is caused by the motion of molecules. The pressure felt due to flow is called dynamic pressure. These two pressures combine to make up total pressure.

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20
Q

Explain and define head loss

A

It is the conversion of fluid pressure and velocity to heat
energy through friction.

Hf = Wf / m = u2 - u1

  • Hf = head loss (friction head) due to fluid friction (ft)
  • Wf = work done against fluid friction (ft lbf)
  • m = mass (lbm)
  • u2 = specific internal energy exiting system (Btu/lbm)
  • u1 = specific internal energy entering system (Btu/lbm)
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21
Q

Explain the effects on head loss from viscosity

A

(Hf) represents the energy used in overcoming fluid friction. Although this represents a loss of energy from the standpoint of fluid flow, it does not normally represent a loss of total energy from the fluid.

Although the total head of the working fluid decreases because of fluid friction, the internal energy of the fluid, as reflected by its temperature, increases. In an insulated pipe in which there is no heat loss to the surroundings, the head loss equals the internal energy gain.

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22
Q

Discuss operational consideration of viscosity as related to head loss

A

Experimental studies of the flow of liquids in pipes showed that the head loss due to fluid friction varies:

  1. Directly with the length of the pipe, since a longer pipe has more surface area
  2. Inversely with the diameter of the pipe, since a pipe with a larger diameter has less surface area per unit of cross-sectional area than a pipe with a smaller diameter.
  3. Directly with the velocity head of the fluid
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23
Q

What is the formula for head loss (Hf) due to friction?

A
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24
Q

Explain and define pump head

A
Pump head (H<sub>p</sub>) is the head added by the pump to each pound of fluid to maintain
or increase its pressure or velocity.

Hp = Wp / m = h2 - h1

H<sub>p</sub> = head added by the pump (ft)
W<sub>p</sub> = work done on the fluid by the pump (ft lbf)
h<sub>2</sub> = specific enthalpy exiting the pump (Btu/lbm)
h<sub>1</sub> = specific enthalpy entering the pump (Btu/lbm)

Specific enthalpy of a working fluid, h, is a property of the fluid which is defined as: h=u+P v where, u= Specific internal energy P= Pressure v= Specific volume

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25
Q

What is Bernoulli’s equation with terms for the work done against fluid friction and work of the pump?

A
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26
Q

What is the Reynolds Number

A

The experimental investigations of Osborne Reynolds in 1883 indicated that for an
noncompressible fluid completely filling a pipe, the mode of flow is determined by:

  • Average velocity of the fluid (Vav)
  • Diameter of the pipe (d)
  • Kinematic viscosity (ν).

Unit analysis, confirmed by experiment, showed that these variables could be grouped to form a unit-less constant called the Reynolds number (NRe) which can be used to determine the mode of flow.

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27
Q

What is the formula for Reynolds Number?

A
28
Q

For Reynolds numbers less than 2000, what flow is present?

A

Laminar Flow

29
Q

For Reynolds numbers greater than 3500, what flow is present?

A

Turbulent Flow

30
Q

For Reynolds numbers between 2,000 and 3,500, what flow is present?

A

Transitional flow.

31
Q

Describe the relationship between Reynolds number and friction factor.

A

The value of the friction factor depends on the Reynolds number and the roughness of the pipe.

With laminar flow, the friction factor does not depend on the relative roughness. It is a function of the Reynolds number only.

For Reynolds numbers greater than about 3,500, where turbulent flow prevails, the friction factor is a function of both the Reynolds number and the relative roughness

32
Q

Explain the effects on head loss from friction factor and relative roughness.

A

The presence of valves and fittings in a line increases the head losses due to fluid friction.

The primary effect of fluid friction and the associated head loss it causes is a pressure drop.

The total head loss is the total energy lost by each lbm of the fluid as it flows through the system. Thus, the fluid exits the system with less flow energy per pound mass than when it entered.

33
Q

Describe fluid flow measurement devices.

A

The most commonly used types are based on the indirect determination of
flow rate using differential pressure measurements. There are several devices commonly used to convert a measured differential pressure into a flow rate. Most of these devices can be classified as one of three basic designs:

  1. pitot tube
  2. venturi meter
  3. orifice meter
34
Q

What is a Pitot Tube?

A

A pitot tube compares the pressure at points 1 and 2. The pressure of point 1 is the total pressure. Recall that total pressure is equal to dynamic pressure plus static pressure. The pressure at point 2 is due to static pressure at the sensing point. The static pressures at points 1 and 2 balance out, resulting in the difference in
pressure being equal to the dynamic pressure. Assuming all kinetic energy at point 1 is converted to dynamic pressure allows the use of Bernoulli’s equation to determine velocity. It must also be assumed there is no height difference at the point where pressures are sampled.

35
Q

Calculate Velocity from D/P

A
36
Q

What is a venturi tube for flow measurement?

A

A venturi meter is another device used to measure flow. It consists of specially constructed converging and diverging pipe sections,

37
Q

What is the formula for calculating flow through a Venturi?

A
38
Q

What is an Orifice Meter?

A
39
Q

Explain why flow measurements must be corrected for density changes.

A

Not only does density vary inversely with temperature, but the magnitude of the change in density increases as temperature increases. Where the temperature of
the measured fluid changes, flow measurement circuitry uses the mass flow rate continuity equation which allows for density compensation.

40
Q

What is the two-phase flow friction multiplier?

A

Two-phase flow friction is greater than singlephase flow friction for the same pipe dimensions and mass flow rate. The difference appears to be a function of the type of flow and results from increased flow speeds.

R = Hf two-phase / Hf sat liquid

Where:
R = two-phase flow friction multiplier (no units)
Hf two-phase = two-phase flow head loss due to friction (ft)
Hf sat liquid = single-phase saturated liquid flow head loss due to friction (ft)

41
Q

What is Slip Ratio?

A

The average velocities of the two phases are not the same. The average velocity of the liquid phase (Vav f) is less than the average velocity of the vapor phase

The slip ratio (SR) of a two-phase flow is a measure of the relative velocities of the liquid and vapor portions.

SR = Vav g / Vav f
Where:
SR = slip ratio (no units)
Vav g = average velocity of the vapor phase (ft/sec)
Vav f = average velocity of the liquid phase (ft/sec)

(Vav g)

42
Q

Explain the purpose of pumps

A

A pump supplies discharge head to make up for head losses and provide a flow rate.

43
Q

Explain the principles of operation of a centrifugal pump.

A

It imparts energy to the fluid in its rotor from centrifugal action. Specifically, Fluid enters the impeller in the central portion, called the eye, flows radially outward, and is discharged around the entire circumference into a casing. While flowing through the rotating impeller, the fluid receives kinetic energy from the vanes. This increases both fluid pressure and velocity. Kinetic energy is a large component of
the total energy of the fluid leaving the impeller. It is necessary to reduce fluid velocity and transform a large part of this velocity head into pressure head. This is usually done in the volute casing surrounding the impeller. The area of the volute increases in the direction of flow. Therefore, to maintain a constant flow rate (i.e.
satisfy the continuity equation), the velocity must decrease. Then, from Bernoulli’s equation, as the velocity head decreases, the pressure head increases, and the total head remains constant. Kinetic energy at the exit of the impeller is
converted to flow energy in the volute casing asvelocity decreases and pressure increases.

44
Q

Discuss how the volute acts to decrease flow velocity and increase outlet pressure.

A
45
Q

Describe how flow rates are controlled for systems containing centrifugal pumps.

A

The capacity, or flow rate, of a single speed centrifugal pump is
controlled by varying the position of a valve on the discharge side of the pump. A variable speed pump varies the output capacity by changing speeds. Throttling a discharge valve can also be used to change the capacity of a variable speed
centrifugal pump.

46
Q

Define and explain cavitation.

A

Cavitation is the formation of vapor bubbles in low pressure fluid flow areas and their subsequent collapse as regions of higher pressure are entered.

47
Q

Define and explain Net Positive Suction Head (NPSH) required and available.

A

The difference between the pump inlet, or suction, pressure and the saturation pressure of the liquid being pumped is called available net positive suction head (NPSH). The required NPSH is the amount of NPSH which must be provided to prevent cavitation, and is determined by the pump manufacturer. If available NPSH is
not greater than required NPSH, the pump will cavitate.

48
Q

Calculate available net positive suction head.

A
49
Q

What is Recirculation Ratio?

A

In a steam generator the mixing of the incoming feedwater with the moisture removed by the moisture separators minimizes the temperature difference between the feedwater inlet nozzle and the steam generator shell, which minimizes thermal stress on the nozzles and steam generator shell. It is an additional pre-heating of feedwater before it reaches the tube bundle region.

The ratio of recirculated moisture to the amount of feedwater supplied (and steam produced) is called the recirculation ratio. Under normal conditions, the recirculation ratio is about three-to-one at full power.

50
Q

What is gas binding?

A

Gas binding is a term used when a pump is filled
with a gas, normally air, instead of the liquid
being pumped. Gas binding is defined as
“excessive air or gas buildup inside a pump
casing”. Under these conditions, the pump
cannot pump the desired liquid. Venting and
filling the pump casing usually eliminate the
problem with gas binding.

51
Q

What is Axial Thrust?

A

Axial thrust results from unbalanced forces acting along the axis of a pump impeller. These unbalanced forces are caused by the difference between the suction pressure, experienced on one side of the impeller, and the discharge pressure
on the other side. Additionally, differences in the surface area exposed to these pressures contributes to axial thrust. These forces are compensated for by using axial thrust bearings or pressure equalizing holes between regions of uneven hydraulic pressure.

52
Q

What is pump runout?

A

Pump runout is the term used to describe a
centrifugal pump when it is pumping at its
maximum capacity. This normally occurs when
system pressure drops to its minimum.

53
Q

What is shutoff head?

A

Shutoff head is the term used when a centrifugal
pump is pumping its fluid with a shut discharge
valve, or against a system pressure equal to or
higher than the pump discharge pressure.

54
Q

Explain how operating a centrifugal pump at shutoff head may cause overheating and describe the methods used to avoid overheating.

A

The pump adds energy to the liquid in the pump casing, causing the liquid (and pump) temperature to rise. If adequate cooling is not provided, liquid temperature eventually reaches the saturation temperature for the pump suction pressure, causing cavitation and possible damage to the pump. The increased temperature of the pump could also lead to bearing damage or inadequate clearances between moving parts, thus damaging the pump. Most pumps are protected against running at shutoff head by a piping system made of a small diameter pipe and/or an orifice. This minimum flow line taps off between the pump and its discharge valve, and normally returns flow back to the suction source.

55
Q

Describe how flow rates are controlled in systems

containing positive displacement pumps.

A

Varying the speed of the stroke or varying the length of the stroke.

56
Q

Discuss the relationship between pump speed, head, flow and power without using formulas or calculations.

A

A plot of discharge head versus capacity, for a given pump speed, is often called the pump characteristic curve.

If the pump speeds up, the entire characteristic curve moves outward, away from the origin. The pump capacity increases by the same factor by which the speed increases, and the pump discharge head increases as the square of the factor by which the speed increases. If the pump operates at constant efficiency, the power required to operate the pump at a new speed increases as the cube of the
factor by which the speed increases.

57
Q

Explain the reason for the shape of a centrifugal pump characteristic curve.

A

the capacity of a centrifugal pump decreases as
the pressure at the pump discharge increases. At
a particular pressure, called the shutoff head, the
pump moves no fluid at all. If the pump
discharges directly to the atmosphere, the pump
capacity is maximum, called pump runout.

58
Q

Describe how a centrifugal pump chracteristic curve will change with pump speed.

A

If the pump speeds up, the entire characteristic
curve moves outward, away from the origin.

59
Q

Discuss the characteristic curve for a typical positive displacement pump, and explain the reason for its shape.

A

A positive displacement pump provides a constant volumetric flow rate as friction losses increase for the same pump speed. The pump head supplied can take any value at constant flow rate.

When friction losses are high, a backpressure builds up in the system, and some high pressure fluid leaks within the pump. Thus, the actual characteristic curve bends to the left at the top, indicating that net flow rate begins to decrease
slightly at some point.

60
Q

Using centrifugal pump characteristic curve and a system chracteristic curve, illustrate how the system operating point changes
due to system throttle valve operation.

A

The system characteristic curve can be drawn on the same graph as the pump characteristic curve. The point where the curves intersect is the point where pump head equals friction loss. This is where the pump operates, and is thus known as
the operating point.

Partially closing a valve in the flow line increases friction losses and moves the system characteristic curve to the left. A centrifugal pump responds by seeking the operating point. Therefore, the pump head increases and the flow rate decreases. Reopening the valve decreases head loss, and moves the system characteristic
curve back to the right.

61
Q

Explain the results of putting centrifugal pumps in series or parallel combinations.

A

The characteristic curve for two identical pumps operating in series is
formed by adding the individual pump heads for a given pump capacity.

The characteristic curve for two pumps operating in parallel is found by adding the
individual pump capacities for the given total heads.

62
Q

Evaluate the head added by a pump to determine
pump efficiency and real and ideal work of the pump.

A

Thus, the head added by a pump (Hp) is a
measure of the pressure rise across the pump.
Pump head is also a measure of the work done
on the fluid by the pump.

See equations…. pgs 43/44

63
Q

Explain the operational implication of water (fluid) hammer.

A

The best prevention of water hammer is the
THINKING OPERATOR. Operators should
consider the possibility of water hammer
occurring before performing any actions which
could cause a water hammer, especially in offnormal
operating conditions, and take steps to
prevent it.

64
Q

Define and explain a Pressure Spike and pipe whip.

A

Water hammer may be observed as a system “pressure spike” – a sudden increase in pressure due to energy in the system encountering obstructions.

The uncontrolled movement of pipes/pumps is called “pipe whip”.

65
Q

Explain the importace of proper system venting for pump operation.

A

Centrifugal pumps are provided with high point
casing vents. The vents allow the pump to be
primed, and to remove the noncondensable gases
that could be trapped in the casing. When a
system is initially filled, the casing vents should
be open before starting the pump, and left open
until a solid stream of liquid comes out.

66
Q

Describe the problems that will occur in Emergency Core Cooling Systems if the pumps are operated at lower than design flow for extended periods of time.

A

A centrifugal pump should not be operated for extended periods of time at shutoff head. This is especially true for the Emergency Core Cooling System (ECCS) pumps. These pumps could be damaged if run for an extended period of time
with lower than design flow.

The pump adds energy to the liquid in the pump casing, causing the liquid (and pump) temperature to rise. If adequate cooling is not provided, liquid temperature eventually reaches the saturation temperature for the pump suction pressure, causing cavitation and possible damage to the pump. The increased temperature of the pump could also lead to bearing damage or inadequate clearances between moving parts, thus damaging the pump.