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Mach numbers | Mechanical waves and sound | Physics | Khan Academy
Mach numbers | Mechanical waves and sound | Physics | Khan Academy
Published: 2010/06/07
Channel: Khan Academy
Mach number
Mach number
Published: 2015/10/27
Channel: Shivam Soni
Mach Number
Mach Number
Published: 2016/04/12
Channel: Aviation English.club
Compressible Flow: Mach Number, Characteristic Mach Number and Stagnation properties
Compressible Flow: Mach Number, Characteristic Mach Number and Stagnation properties
Published: 2016/03/25
Channel: Alpesh Panchal
Mach Number | Mechanical Engineering | Chegg Tutors
Mach Number | Mechanical Engineering | Chegg Tutors
Published: 2016/04/19
Channel: Chegg
What is Mach Number?
What is Mach Number?
Published: 2017/02/11
Channel: Tahir Javed
Mod-01 Lec-04 Lecture-04-The Mach Number and Compressible Flow
Mod-01 Lec-04 Lecture-04-The Mach Number and Compressible Flow
Published: 2012/07/20
Channel: nptelhrd
Critical Mach Number (Mcrit)
Critical Mach Number (Mcrit)
Published: 2015/01/07
Channel: Dfan 315
Mach number
Mach number
Published: 2014/05/08
Channel: encyclopediacc
What Is Mach Speed?
What Is Mach Speed?
Published: 2015/08/05
Channel: TestTube 101
Mach number Meaning
Mach number Meaning
Published: 2015/04/20
Channel: SDictionary
Mach Number
Mach Number
Published: 2015/01/07
Channel: Dfan 315
Crash Course: Swept Wings
Crash Course: Swept Wings
Published: 2015/06/30
Channel: Boldmethod
Explained: Critical Mach Number [Airplanes]
Explained: Critical Mach Number [Airplanes]
Published: 2013/06/12
Channel: JoshTheEngineer
Mach Number. Subsonic, Transonic and Supersonic flows
Mach Number. Subsonic, Transonic and Supersonic flows
Published: 2017/03/07
Channel: FluidDynamics
F-18 Super Hornet .9 Mach - High Speed
F-18 Super Hornet .9 Mach - High Speed
Published: 2011/10/17
Channel: High Tech Corvette
Calc air converging diverging nozzle Mach 1p5
Calc air converging diverging nozzle Mach 1p5
Published: 2014/02/25
Channel: Randall Manteufel
CRP-5: Mach number & the speed of sound
CRP-5: Mach number & the speed of sound
Published: 2016/04/07
Channel: GoPro Flying
Mach number
Mach number
Published: 2016/01/22
Channel: WikiAudio
Supersonic Flow - Mach Number
Supersonic Flow - Mach Number
Published: 2015/11/20
Channel: Jaime Martínez
Explained: Area-Mach Number Relation
Explained: Area-Mach Number Relation
Published: 2017/03/06
Channel: JoshTheEngineer
Compressible flow through Nozzles
Compressible flow through Nozzles
Published: 2016/02/11
Channel: Amit Mandal
Derive equation for sonic speed and discuss mach number
Derive equation for sonic speed and discuss mach number
Published: 2014/02/25
Channel: Randall Manteufel
FLYING ABOVE SPEED OF SOUND MACH One HIGH SPEED FLIGHT
FLYING ABOVE SPEED OF SOUND MACH One HIGH SPEED FLIGHT
Published: 2016/08/31
Channel: ZIG ZAG
Mach Number
Mach Number
Published: 2012/05/26
Channel: kingrams1
E6B Flight Computer: Mach Number to KTS
E6B Flight Computer: Mach Number to KTS
Published: 2010/12/11
Channel: Flight Tutor
What is CRITICAL MACH NUMBER? What does CRITICAL MACH NUMBER mean?
What is CRITICAL MACH NUMBER? What does CRITICAL MACH NUMBER mean?
Published: 2017/06/10
Channel: The Audiopedia
35 compressibility
35 compressibility
Published: 2011/08/22
Channel: Guy Riefler
Machmeter, Mach, TAS, CAS Relationship
Machmeter, Mach, TAS, CAS Relationship
Published: 2016/04/12
Channel: Aviation English.club
What does Mach number mean?
What does Mach number mean?
Published: 2015/04/01
Channel: What Does That Mean?
YUGIOH- AMV Yuma Vs Mach (Number 44)
YUGIOH- AMV Yuma Vs Mach (Number 44)
Published: 2016/10/11
Channel: AMV YUGIOH HA
How To Calculate True Air Speed (TAS) From A Mach Number | AviaTube Aviation Briefings
How To Calculate True Air Speed (TAS) From A Mach Number | AviaTube Aviation Briefings
Published: 2013/09/11
Channel: AviaTube
what is the use of mach number  | gas dynamics interview tips | wikitechy.com
what is the use of mach number | gas dynamics interview tips | wikitechy.com
Published: 2016/08/19
Channel: Wikitechy Technology Tutorials
High Speed Flight
High Speed Flight
Published: 2016/05/23
Channel: Planes Over Head
CPL | ATPL CBT | PRINCIPAL OF FLIGHT | HIGH SPEED FLIGHT | MACH NUMBER | CRITICAL MACH NUMBER
CPL | ATPL CBT | PRINCIPAL OF FLIGHT | HIGH SPEED FLIGHT | MACH NUMBER | CRITICAL MACH NUMBER
Published: 2017/04/02
Channel: サチン
mach number derivation | compressible flow lectures | fluid dynamics | choking in nozzle | fluid
mach number derivation | compressible flow lectures | fluid dynamics | choking in nozzle | fluid
Published: 2017/04/20
Channel: MECHANICAL ENGINEERING EXPLAINED OFFICIAL
ANSYS CFX - De Laval Nozzle - Mach Number - CFD Simulation
ANSYS CFX - De Laval Nozzle - Mach Number - CFD Simulation
Published: 2014/10/17
Channel: CFD.NINJA ANSYS
Mach Number
Mach Number
Published: 2016/04/27
Channel: Joseph Dallaire
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mach number
Published: 2015/11/12
Channel: Jaime Martínez
How To: Find Mach Number from a Picture (Part 1)
How To: Find Mach Number from a Picture (Part 1)
Published: 2016/01/19
Channel: JoshTheEngineer
The Relationship Between Aircraft CL Alpha & Mach Number
The Relationship Between Aircraft CL Alpha & Mach Number
Published: 2017/06/09
Channel: Tamarack Aerospace Group
MACH vs IAS
MACH vs IAS
Published: 2010/10/15
Channel: maxsmodels
Conversing diversing nozzle and mach number explained
Conversing diversing nozzle and mach number explained
Published: 2017/04/09
Channel: Tech point
supersonic flow pas a cube (Mach number)
supersonic flow pas a cube (Mach number)
Published: 2013/10/29
Channel: OpenSourceMeshing
Mach number - External compressible flow over supersonic airfoil
Mach number - External compressible flow over supersonic airfoil
Published: 2015/11/20
Channel: Pedro Pérez
Mach-number - solar surface convection simulation
Mach-number - solar surface convection simulation
Published: 2014/09/01
Channel: Zaz Mag
Hazards Of High Mach Flight
Hazards Of High Mach Flight
Published: 2014/04/03
Channel: capncrunch8942 dorf
War Thunder Me-163 Secretly goes nearly mach 2. WOW
War Thunder Me-163 Secretly goes nearly mach 2. WOW
Published: 2014/03/06
Channel: Jnorbz247
War Thunder - Me 163 Breaching Mach 1
War Thunder - Me 163 Breaching Mach 1
Published: 2013/03/09
Channel: BigPooprr
Reaching Mach 1: What It Feels Like to Break the Sound Barrier
Reaching Mach 1: What It Feels Like to Break the Sound Barrier
Published: 2016/03/18
Channel: Great Big Story
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WIKIPEDIA ARTICLE

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An F/A-18 Hornet creating a vapor cone at transonic speed just before reaching the speed of sound

In fluid dynamics, the Mach number (M or Ma) (/mɑːx/; German: [maχ]) is a dimensionless quantity representing the ratio of flow velocity past a boundary to the local speed of sound.[1][2]

where:

M is the Mach number,
u is the local flow velocity with respect to the boundaries (either internal, such as an object immersed in the flow, or external, like a channel), and
c is the speed of sound in the medium.

By definition, Mach 1 is equal to the speed of sound. Mach 0.65 is 65% of the speed of sound (subsonic), and Mach 1.35 is 35% faster than the speed of sound (supersonic).

The local speed of sound, and thereby the Mach number, depends on the condition of the surrounding medium, in particular the temperature. The Mach number is primarily used to determine the approximation with which a flow can be treated as an incompressible flow. The medium can be a gas or a liquid. The boundary can be traveling in the medium, or it can be stationary while the medium flows along it, or they can both be moving, with different velocities: what matters is their relative velocity with respect to each other. The boundary can be the boundary of an object immersed in the medium, or of a channel such as a nozzle, diffusers or wind tunnels channeling the medium. As the Mach number is defined as the ratio of two speeds, it is a dimensionless number. If M < 0.2–0.3 and the flow is quasi-steady and isothermal, compressibility effects will be small and simplified incompressible flow equations can be used.[1][2]

The Mach number is named after Austrian physicist and philosopher Ernst Mach, and is a designation proposed by aeronautical engineer Jakob Ackeret. As the Mach number is a dimensionless quantity rather than a unit of measure, with Mach, the number comes after the unit; the second Mach number is "Mach 2" instead of "2 Mach" (or Machs). This is somewhat reminiscent of the early modern ocean sounding unit "mark" (a synonym for fathom), which was also unit-first, and may have influenced the use of the term Mach. In the decade preceding faster-than-sound human flight, aeronautical engineers referred to the speed of sound as Mach's number, never "Mach 1."[3]

Overview[edit]

Mach number is useful because the fluid behaves in a similar manner at a given Mach number, regardless of other variables.[4] As modeled in the International Standard Atmosphere, dry air at mean sea level, standard temperature of 15 °C (59 °F), the speed of sound is 340.3 meters per second (1,116.5 ft/s).[5] The speed of sound is not a constant; in a gas, it increases as the absolute temperature increases, and since atmospheric temperature generally decreases with increasing altitude between sea level and 11,000 meters (36,089 ft), the speed of sound also decreases. For example, the standard atmosphere model lapses temperature to −56.5 °C (−69.7 °F) at 11,000 meters (36,089 ft) altitude, with a corresponding speed of sound (Mach 1) of 295.0 meters per second (967.8 ft/s), 86.7% of the sea level value.

Classification of Mach regimes[edit]

While the terms "subsonic" and "supersonic," in the purest sense, refer to speeds below and above the local speed of sound respectively, aerodynamicists often use the same terms to talk about particular ranges of Mach values. This occurs because of the presence of a "transonic regime" around M = 1 where approximations of the Navier-Stokes equations used for subsonic design actually no longer apply; the simplest explanation is that the flow locally begins to exceed M = 1 even though the freestream Mach number is below this value.

Meanwhile, the "supersonic regime" is usually used to talk about the set of Mach numbers for which linearised theory may be used, where for example the (air) flow is not chemically reacting, and where heat-transfer between air and vehicle may be reasonably neglected in calculations.

In the following table, the "regimes" or "ranges of Mach values" are referred to, and not the "pure" meanings of the words "subsonic" and "supersonic".

Generally, NASA defines "high" hypersonic as any Mach number from 10 to 25, and re-entry speeds as anything greater than Mach 25. Aircraft operating in this regime include the Space Shuttle and various space planes in development.

Regime Mach knots mph km/h m/s General plane characteristics
Subsonic <0.8 <530 <609 <980 <273 Most often propeller-driven and commercial turbofan aircraft with high aspect-ratio (slender) wings, and rounded features like the nose and leading edges.
Transonic 0.8-1.2 530-794 609-914 980-1,470 273-409 Transonic aircraft nearly always have swept wings, causing the delay of drag-divergence, and often feature a design that adheres to the principles of the Whitcomb Area rule.
Supersonic 1.2–5.0 794-3,308 915-3,806 1,470–6,126 410–1,702 Aircraft designed to fly at supersonic speeds show large differences in their aerodynamic design because of the radical differences in the behaviour of flows above Mach 1. Sharp edges, thin aerofoil-sections, and all-moving tailplane/canards are common. Modern combat aircraft must compromise in order to maintain low-speed handling; "true" supersonic designs include the F-104 Starfighter, SR-71 Blackbird and BAC/Aérospatiale Concorde.
Hypersonic 5.0–10.0 3,308-6,615 3,806–7,680 6,126–12,251 1,702–3,403 The X-15, at Mach 6.72 is one of the fastest manned aircraft. Also, cooled nickel-titanium skin; highly integrated (due to domination of interference effects: non-linear behaviour means that superposition of results for separate components is invalid), small wings, such as those on the Mach 5 X-51A Waverider
High-hypersonic 10.0–25.0 6,615-16,537 7,680–19,031 12,251–30,626 3,403–8,508 The NASA X-43, at Mach 9.6 is one of the fastest aircraft. Thermal control becomes a dominant design consideration. Structure must either be designed to operate hot, or be protected by special silicate tiles or similar. Chemically reacting flow can also cause corrosion of the vehicle's skin, with free-atomic oxygen featuring in very high-speed flows. Hypersonic designs are often forced into blunt configurations because of the aerodynamic heating rising with a reduced radius of curvature.
Re-entry speeds >25.0 >16,537 >19,031 >30,626 >8,508 Ablative heat shield; small or no wings; blunt shape

High-speed flow around objects[edit]

Flight can be roughly classified in six categories:

Regime Subsonic Transonic Sonic Supersonic Hypersonic Hypervelocity
Mach <0.8 0.8–1.2 1.0 1.2–5.0 5.0–10.0 >10.0

For comparison: the required speed for low Earth orbit is approximately 7.5 km/s = Mach 25.4 in air at high altitudes.

At transonic speeds, the flow field around the object includes both sub- and supersonic parts. The transonic period begins when first zones of M > 1 flow appear around the object. In case of an airfoil (such as an aircraft's wing), this typically happens above the wing. Supersonic flow can decelerate back to subsonic only in a normal shock; this typically happens before the trailing edge. (Fig.1a)

As the speed increases, the zone of M > 1 flow increases towards both leading and trailing edges. As M = 1 is reached and passed, the normal shock reaches the trailing edge and becomes a weak oblique shock: the flow decelerates over the shock, but remains supersonic. A normal shock is created ahead of the object, and the only subsonic zone in the flow field is a small area around the object's leading edge. (Fig.1b)

Transsonic flow over airfoil 1.svg Transsonic flow over airfoil 2.svg
(a) (b)

Fig. 1. Mach number in transonic airflow around an airfoil; M < 1 (a) and M > 1 (b).

When an aircraft exceeds Mach 1 (i.e. the sound barrier), a large pressure difference is created just in front of the aircraft. This abrupt pressure difference, called a shock wave, spreads backward and outward from the aircraft in a cone shape (a so-called Mach cone). It is this shock wave that causes the sonic boom heard as a fast moving aircraft travels overhead. A person inside the aircraft will not hear this. The higher the speed, the more narrow the cone; at just over M = 1 it is hardly a cone at all, but closer to a slightly concave plane.

At fully supersonic speed, the shock wave starts to take its cone shape and flow is either completely supersonic, or (in case of a blunt object), only a very small subsonic flow area remains between the object's nose and the shock wave it creates ahead of itself. (In the case of a sharp object, there is no air between the nose and the shock wave: the shock wave starts from the nose.)

As the Mach number increases, so does the strength of the shock wave and the Mach cone becomes increasingly narrow. As the fluid flow crosses the shock wave, its speed is reduced and temperature, pressure, and density increase. The stronger the shock, the greater the changes. At high enough Mach numbers the temperature increases so much over the shock that ionization and dissociation of gas molecules behind the shock wave begin. Such flows are called hypersonic.

It is clear that any object traveling at hypersonic speeds will likewise be exposed to the same extreme temperatures as the gas behind the nose shock wave, and hence choice of heat-resistant materials becomes important.

High-speed flow in a channel[edit]

As a flow in a channel becomes supersonic, one significant change takes place. The conservation of mass flow rate leads one to expect that contracting the flow channel would increase the flow speed (i.e. making the channel narrower results in faster air flow) and at subsonic speeds this holds true. However, once the flow becomes supersonic, the relationship of flow area and speed is reversed: expanding the channel actually increases the speed.

The obvious result is that in order to accelerate a flow to supersonic, one needs a convergent-divergent nozzle, where the converging section accelerates the flow to sonic speeds, and the diverging section continues the acceleration. Such nozzles are called de Laval nozzles and in extreme cases they are able to reach hypersonic speeds (Mach 13 (15,926 km/h; 9,896 mph) at 20 °C).

An aircraft Machmeter or electronic flight information system (EFIS) can display Mach number derived from stagnation pressure (pitot tube) and static pressure.

Calculation[edit]

The Mach number at which an aircraft is flying can be calculated by

where:

M is the Mach number
u is velocity of the moving aircraft and
c is the speed of sound at the given altitude

Note that the dynamic pressure can be found as:

Assuming air to be an ideal gas, the formula to compute Mach number in a subsonic compressible flow is derived from Bernoulli's equation for M < 1:[6]

where:

qc is impact pressure (dynamic pressure) and
p is static pressure
is the ratio of specific heat of a gas at a constant pressure to heat at a constant volume (1.4 for air).

The formula to compute Mach number in a supersonic compressible flow is derived from the Rayleigh supersonic pitot equation:

Calculating Mach number from pitot tube pressure[edit]

Mach number is a function of temperature and true airspeed. Aircraft flight instruments, however, operate using pressure differential to compute Mach number, not temperature.

Assuming air to be an ideal gas, the formula to compute Mach number in a subsonic compressible flow is found from Bernoulli's equation for M < 1 (above):[6]

The formula to compute Mach number in a supersonic compressible flow can be found from the Rayleigh supersonic pitot equation (above) using parameters for air:

where:

qc is the dynamic pressure measured behind a normal shock.

As can be seen, M appears on both sides of the equation. The easiest method to solve the supersonic M calculation is to enter both the subsonic and supersonic equations into a computer spreadsheet such as Microsoft Excel, OpenOffice.org Calc, or some equivalent program to solve it numerically. It is first determined whether M is indeed greater than 1.0 by calculating M from the subsonic equation. If M is greater than 1.0 at that point, then the value of M from the subsonic equation is used as the initial condition in the supersonic equation. Then a simple iteration of the supersonic equation is performed, each time using the last computed value of M, until M converges to a value—usually in just a few iterations.[6] Alternatively, Newton's method can also be used.

See also[edit]

Notes[edit]

  1. ^ a b Young, Donald F.; Bruce R. Munson; Theodore H. Okiishi; Wade W. Huebsch (2010). A Brief Introduction to Fluid Mechanics (5 ed.). John Wiley & Sons. p. 95. ISBN 978-0-470-59679-1. 
  2. ^ a b Graebel, W.P. (2001). Engineering Fluid Mechanics. Taylor & Francis. p. 16. ISBN 978-1-56032-733-2. 
  3. ^ Bodie, Warren M., The Lockheed P-38 Lightning, Widewing Publications ISBN 0-9629359-0-5.
  4. ^ Nancy Hall (ed.). "Mach Number". NASA. 
  5. ^ Clancy, L.J. (1975), Aerodynamics, Table 1, Pitman Publishing London, ISBN 0-273-01120-0
  6. ^ a b c Olson, Wayne M. (2002). "AFFTC-TIH-99-02, Aircraft Performance Flight Testing." (PDF). Air Force Flight Test Center, Edwards AFB, CA, United States Air Force. Archived September 4, 2011, at the Wayback Machine.

External links[edit]

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