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Lecture 7 Demos: U-tube manomoter, Archimedes principle, const fluid height, venturi flowmeter.

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Presentation on theme: "Lecture 7 Demos: U-tube manomoter, Archimedes principle, const fluid height, venturi flowmeter."— Presentation transcript:

1 Lecture 7 Demos: U-tube manomoter, Archimedes principle, const fluid height, venturi flowmeter.

2 Mechanical sensors: motivations. How do we predict materials failure? Aircraft wings (DC-10 metal fatigue: the wings suddenly fell off) Predict cracks and collapse in bridges and buildings Strength is the ability to withstand force or stress Remember stress=force/area

3 How do we measure fluid flow? Beer taps-want to avoid losing the bubbles Grain silos-want to predict the rate of static buildup to avoid explosions, yet maximize the throughput Chemical reactions- want to ensure fluids properly mixed Usually want laminar flow, not turbulent.

4 Mechanical Sensors Mechanical sensors react to stimuli via some mechanical effect The output may be: Mechanical (e.g. a dial or fluid level) or Electrical (e.g. a voltage or current) Definitions Force and pressure sensors Basic pressure sensors Medical pressure measurement systems Flow and flow-rate sensors. Overview:

5 Force and Pressure Sensors How do we measure an unknown force? Acceleration Method Apply force to known mass, measure acceleration. Example: Force on Pendulum, apply force measure deflection.

6 How do we measure hydrostatic pressure in fluids and liquids? Blood/brain/spinal fluid pressure-how do we measure non-invasively? Hydraulic systems-bulldozer arms, car disk brakes/hydraulic lifts How do divers know how much air they have left in their tanks?

7 Pressure sensors: How do we tell when someone is walking down a corridor? How can we weigh trucks as they pass over a road?

8 Force and Pressure Sensors Gravity balance method. Compare unknown force with action of gravitational force. Example: Balance scale. (zero-balance method)





13 Spring Method Use force to stretch or compress a spring of known strength, and measure displacement: F=kx, k is the spring constant. Example: Fruit scales at supermarket

14 Pressure-sensing method. Convert the unknown force to a fluid pressure, which is converted using a pressure sensor. Also known as deadweight sensor-used for weight calibrations.

15 From H. Norton, ‘Sensor and analyzer handbook’ Note that these all convert a pressure into an angular or linear displacement. We can then sense the displacement eledctronically or optically. Some pressure sensing elements

16 Pressure reference configurations

17 If force is constant, pressure is static or hydrostatic: Beer in (untapped) keg Butane gas bottle. If force is varying, pressure is dynamic or hydrodynamic: Arterial blood pressure. Units of Pressure: 1 Pascal = 1 Newton/m 2 1 atm (Atmospheric pressure) = 101325 Pa 760 torr = 1 atm Pressure-sensing method.

18 Pascal’s Principle Pressure applied to an enclosed system is transmitted undiminished to every portion of the fluid and container walls. This is the basis of all hydraulics: a small pressure can be made to exert a large force by changing the dimensions of the vessel

19 Applications of Pascal’s Principle Disk brakes Car Lift Medical applications

20 Notes on Pascal’s principle Pascal’s principle neglects the effects of gravity-need to add the contribution ρgh where ρ is the density, g the acceleration due to gravity, and h the height of the fluid. Also, only true in hydrodynamic systems if change is quasi-static. Quasi-static means that after a small change is made, turbulence is allowed to die down then measurement is made. Examples are hydrodynamic systems where flow is non-turbulent and the pipe orifice is small compared with its length.

21 Bourdon tube sensor Bourdon tube pressure sensor: curved or twisted tube, sealed at one end. Measure resistance change as the pressure in the active tube is changed Can be directly calibrated in Torr As pressure inside changes, tube uncurls; this displacement can be transduced using a variable sliding resistior

22 Membrane pressure sensors Subdivided into bellows, thin plate and diaphragm sensors. These work by measuring the deflection of a solid object by an external pressure. This displacement is then measured, and converted into a pressure reading Membrane sensors can be made very small using micromachining; called microelectromechanical systems (MEMS). We will be discussing MEMS in more detail later.

23 Some MEMS sensors 1 μm high MEMs capacitive accelerometer: such devices are at the heart of car airbags. Machined out of single silicon wafer ‘Proof mass’ is freer to move in response to acceleration forces Images from MEMs gyroscope based on ‘tuning fork’ design

24 Medical pressure measurement. This is a major application for sensor technology. Most common measurement is for blood pressure. More fully: Inter-cardiac blood pressure Arterial blood pressure Spinal fluid pressure Central venous pressure Pulmonary artery pressure Venous blood pressure Intraventricular brain pressure The difference in these measurements is the range of measurement; we can often use the same sensor for different measurements

25 Medical students are often told there is an “Ohm’s law for blood” P=F.R, Where: P is pressure difference in torr. F is flow rate in millilitres/second. R is blood vessel resistance in “periphial resistance units” (PRU) where 1 PRU allows a flow of 1 ml/s under 1 torr pressure. This is misleading: in fact, blood vessels change diameter from systemic adjustments and from pulsatile pressure wave. minimally invasive sterile electrically insulated Medical sensors should be: Medical pressure sensors

26 In fact, the flow rate is better given by Poiseuille’s Law: Where: F is flow in cubic centimetres/second P is Pressure in dynes per square centimetre η is coefficient of viscosity in dynes/square centimetre R is vessel radius in centimetre L is vessel length in centimetres

27 Blood Pressure Waveform Four kinds of pressure: T 2 : Peak Pressure (systolic) T f : Minimum pressure (diastolic) Dynamic Average (1/2 peak minus minimum) Average pressure (arterial)

28 Mean arterial pressure is given by: But clinically (for doctors and nurses in a hospital or sleep lab setting) a much simpler approximation is used: Where P 1 is diastolic Pressure and P 2 is systolic pressure Direct measurement of blood pressure is most accurate but also more dangerous (involves poking tubes into arteries, very invasive.) Blood Pressure Analysis

29 Open Tube Manometer Sensing tube tube inserted directly into artery; mercury is poisonous, so need saline buffer Measure pressure by height of sensing column: Only used in intensive care units.  =density of Manometer fluid

30 Sphygmomanometry (Korotkoff Method) Inflatable cuff placed on upper arm and inflated until blood can’t flow Sound sensor (stethoscope) placed downstream Pressure is released When can hear blood squirting (Korotkoff sounds), the cuff pressure equals systolic (higher) pressure Hear continuous but turbulent flow when cuff pressure equals diastolic pressure.

31 The diamond Anvil One way to get huge pressures is to use diamonds to squeeze a sample Can achieve pressures up to 80 GPa (or even higher) So, like, is that big?

32 Pressures are given in Atmospheres 10 -31 |- Non equilibrium "pressure" of hydrogen gas in intergalactic space. 10 -28 |- 10 -25 |- 10 -22 |- Non equilibrium "pressure" of cosmic microwave background radiation. 10 -19 |- Pressure in interplanetary space. 10 -16 |-Best vacuum achieved in laboratory. 10 -13 |- Atmospheric pressure at altitude of 300 miles. 10 -10 |- Pressure of strong sunlight at surface of earth. 10 -8 |- 10 -7 |- Partial pressure of hydrogen in atmosphere at sea level. 10 -6 |-Best vacuum attainable with mechanical pump. Radiation pressure at surface of sun. 10 -5 |-Pressure of the foot of a water strider on a surface of water. Osmotic pressure of sucrose at concentration of 1 milligram per liter. 10 -4 |-Pressure of sound wave at threshold of pain (120 decibels). Partial pressure of carbon dioxide in atmosphere at sea level. 10 -3 |- Vapour pressure of water at triple point of water. 10 -2 |-Overpressure in mouth before release of consonant p. Pressure inside light bulb. 10 -1 |- Atmospheric pressure at summit of Mount Everest. 1 |-Atmospheric pressure at sea level. Pressure of ice skater standing on ice. 10 |-Maximum pressure inside cylinder of high compression engine. Air pressure in high-pressure bicycle tyre. 10 2 |-Steam pressure in boiler of a power plant. Peak pressure of fist on concrete during karate strike. 10 3 |-Pressure at greatest depths in oceans. 10 4 |-Pressure at which mercury solidifies at room temperature. Pressure at which graphite becomes diamond. 10 5 |-Highest pressure attainable in laboratory before diamond anvil cell. Radiation pressure of focused beam of pulsed laser light. 10 6 |-Highest pressure achieved with diamond anvil cell. Pressure at centre of Earth. 10 7 |-Pressure at centre of Saturn. 10 8 |-Pressure at centre of Jupiter. Radiation pressure at centre of sun. 10 10 |- Pressure at centre of sun. 10 13 |- 10 16 |-Pressure at centre of red-giant star. Pressure at centre of white-dwarf star. 10 19 |- 10 22 |- 10 25 |- Pressure at centre of superdense star. 10 28 |- Pressure at centre of neutron star. Relative pressure scale

33 The Holtz cell The Holtz cell is a way to achieve huge pressures in a diamond anvil Uses a simple lever system to apply pressure

34 The diamond Anvil A photo of a working diamond anvil at the institute for transuranic elements, in Europe

35 Lecture 8

36 Flow and Flow rate. Laminar flow: smooth, orderly and regular Turbulent flow: chaotic phenomena (whorls, eddies, vortices) Mechanical sensors have inertia, which can integrate out small variations due to turbulence Flow in a capillary described by Pouiselle’s law.(But beware: only valid for laminar flow) This begs the question: what makes flow laminar or turbulent?

37 Laminar and Turbulent flow Laminar flow is characterised by : smooth flow lines all fluid velocity in same direction flow velocity is zero at tube walls flow speed increases closer to tube center

38 Reynolds Number. Reynold’s Number R Where ρ is the fluid density (kg/m 3 ) V is the mean fluid velocity (m/s) D is the capillary/pipe diameter (m)  is the viscosity of the fluid (Ns/m 2 ) R > 4000, flow is turbulent R < 2000, flow is laminar

39 Flow Sensors Many sensors measure flow rate. Mass flow rate: mass transferred per unit time (kg/s) Volumetric flow rate: volume of material per unit time (m 3 /s) In gas systems, mass and volume rates are expressed in volume flow. Mass flow referenced to STP (standard temperature and pressure) and converted to equivalent volume flow (eg sccm = standard cubic centimetres per minute)

40 Thermal flow Sensor Hot wire anenometer: Cooling of resistive element by fluid flow is measured by Voltmeter

41 Mass Flow controllers Uses two thermometers which supply heat to the gas as well as measuring temperature The faster that the gas flows, the more heat is removed from the upstream thermometer The downstream thermometer also measures the heat flow, increasing accuracy No contact between sensors and gases (no contamination)

42 Photo of a Mass Flow controller Can see that flow direction is important Solid-state valves and interface No moving parts=> no wear Needs to be calibrated for each gas

43 CVD diamond growth reactor

44 Steven’s MFC anecdote

45 Turbulence makes a difference!

46 Different growth patterns with different flows

47 Mechanical obstruction sensors Vane flow meter

48 Some more mechanical obstruction sensors All these sensors turn a change in flow rate into a change in linear or angular displacement

49 Rotating mechanical obstruction sensors sensors (a) and (b) turn a constant flow rate into a constant angular velocity

50 Rotor wheel flow sensor The rotating vane can be attached to a coil in a magnetic field The current generated in the coil is proportional to the flow rate

51 Pressure drop sensors When fluid in a pipe passes through a restriction there is a drop in pressure. Total pressure, P t, after the constriction is P t = P s + P d P s is the static pressure, P d is the dynamic (or impact) pressure P t is sometimes called the stagnation pressure How does this work?

52 Bernoulli’s Equation Where: ρ is the fluid mass density (Ns 2 m -1 ) v is the fluid velocity (m/s) g is the acceleration due to gravity z is the height of fluid (often called head) P is the pressure on the fluid This is equivalent to saying that an element of fluid flowing along a streamline trades speed for height or for pressures A consequence is that as flow velocity increases, the pressure on the vessel walls decreases

53 Differential pressure sensors These sensors change the cross-sectional area A, which increases the velocity v. Since the height of the fluid is constant, the pressure must decrease The amount of material flowing per second does not change, so A 1 v 1 =A 2 v 2 Bernoulli’s equation becomes ½ ρv 1 2 +P 1 = ½ ρv 2 2 +P 2 Combine these expressions to get

54 Differential pressure sensors These sensors change the cross-sectional area A, which increases the velocity v Since the height of the fluid is constant, the pressure must decrease after the obstruction The difference in pressures, combined with the cross-sectional area, tells us the velocity before the obstruction

55 Wire mesh flow sensor Used to measure bubble propagation in gases Uses grid of wires to measure electrical conductivity at wire crossing points





60 Images from wire mesh sensor Note the area of laminar flow Light areas are flowing faster

61 Cannula pressure-drop sensor

62 Ultrasonic flow sensors Ultrasonic waves are sound waves above human hearing (>20 kHz) Typical frequencies are 20 kHz - 20 MHz. Several types of ultrasonic sensors are available- the most common are dynamic or piezoelectric sensors A typical dynamic sensor is a thin, low mass diaphragm, stretched over passive electromagnet. Such diaphragms operates at frequencies up to 100 kHz Good for Doppler shift intruder alarms (demo) Remember that sound waves are longitudinal pressure waves caused by vibrations in a medium

63 Ultrasonic flow sensors Many ultrasonic flow sensors consist of pairs of transducers Each transducer can operate as either a source or a detector of sound waves

64 Dynamic Ultrasonic Sensors As a generator of ultrasonic waves: the drive current creates a magnetic field which pushes against the permanent magnet. As a detector: the motion of the element induces a current in the drive coil

65 Piezoelectric ultrasonic transducers We have encountered piezoelectrics in the context of force sensors An extension of this is the use of piezos to convert the compressions and rarefactions of a sound wave into an electrical signal Deforms a crystalline structure under potential stimulation Operated at resonant frequency (quartz crystal reference) Used in computers and wrist watches as a time reference.

66 Piezoelectric ultrasonic transducers The piezo transmits when an applied potential distorts crystal Receives when pressure wave distorts crystal

67 Measuring the speed of sound in a crystal using ultrasound


69 Ultrasound baby photos ~ads/ultrasound.jpg

70 The Doppler effect We can use the Doppler effect to measure the velocity of a fluid. Doppler effect is a shift in frequency from a moving source of waves.

71 For sound waves reflected off a moving object, there are two shifts: One shift upon receiving the signal, the second upon transmitting. The net shift is given by:  f is the Doppler shifted frequency f is the source frequency v is fluid velocity  the angle between the ultrasonic beam and the fluid velocity c s is the speed of sound in the fluid. The Doppler effect

72 Doppler shift needs “stuff” to reflect off: either optically active molecules (eg Haemoglobin) or turbulence (bubbles) Does not work with pure liquids. Used as a non-invasive blood flow monitor Powerful extra tool when combined with ultra-sonic imaging Notes on the Doppler Shift

73 Doppler Blood measurement Doppler effect can be used to measure variations in blood flow speed Often used for measuring pulses on animals

74 Ultrasonic transit-time flowmeter Transit time T AB between A and B depends on the fluid velocity difference in transit times :  T=T AB -T BA D distance AB between sensors  angle between transit path and flow V is velocity of fluid C s speed of sound in fluid The flow velocity is given by:

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