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A full version program for Android, by One Touch Studio.Have you ever seen someone get a taser shot? It looks so real, doesn't it? With Electric Stun Gun, you can create that same effect. It's so fun to touch and see the shock waves generated by this app. The fun part is that it will also flash your phone's LED flashlight if it's enabled.This app has a built-in taser/stun gun image in the center of the screen. It can be pressed to generate a shock. When you touch the gun, it will generate a crackling sound and vibrate the device. It can be used as a prank to shock your friends and pretend that you have an electric gun that will shock them whenever you touch it.It can be enabled or disabled to turn on/off the electric shock sound and vibration.Program available in other languagesดาวน์โหลด Electric Stun Gun Taser Prank [TH]Descargar Electric Stun Gun Taser Prank [ES]Electric Stun Gun Taser Prank indir [TR]تنزيل Electric Stun Gun Taser Prank [AR]Pobierz Electric Stun Gun Taser Prank [PL]Télécharger Electric Stun Gun Taser Prank [FR]Unduh Electric Stun Gun Taser Prank [ID]Ladda ner Electric Stun Gun Taser Prank [SV]Electric Stun Gun Taser Prank herunterladen [DE]Скачать Electric Stun Gun Taser Prank [RU]Scarica Electric Stun Gun Taser Prank [IT]Electric Stun Gun Taser Prank 다운로드 [KO]Tải xuống Electric Stun Gun Taser Prank [VI]下载Electric Stun Gun Taser Prank [ZH]Download Electric Stun Gun Taser Prank [NL]ダウンロードElectric Stun Gun Taser Prank [JA]Download do Electric Stun Gun Taser Prank [PT]Explore MoreLatest articlesLaws concerning the use of this software vary from country to country. We do not encourage or condone the use of this program if it is in violation of these laws. Zel’dovich YaB, Raizer YuP (1967) Physics of shock waves and high-temperature hydrodynamic phenomena (English translation), vol 2. Academic Press, New York and London, pp 685–784 Google Scholar Davidson L, Shahinpoor M (eds) (1997) High-pressure shock compression of solids I–IV. Springer, New York Google Scholar Bethe H (1942) Theory of shock waves in a medium with arbitrary equation of state. Original paper in report. Republished in: Johnson JN, Cheret R (eds) Classic papers on shock compression science. Springer, London, 1998, pp 421–492 Google Scholar McQueen RG, Marsh SP, Taylor JW, Fritz JN, Carter WJ (1970) High velocity impact phenomena. In: Kinslow R (ed), Chap VII. Academic Press, New York, pp 293–417 Google Scholar Marsh SP (1981) Los Alamos shock Hugoniot data. University of California, Berkeley Google Scholar van Thiel M (1966) Compendium of shock wave data. University of California Press, Livermore, CA Google Scholar Entrance page to shock wave database (2002)Decarli PS, Jamieson JC (1961) Formation of diamond by explosive shock. Science 133:1821–1822Article ADS Google Scholar Prümmer R (2006) Explosive compaction of powders and composites. CRC Press, BerlinBook Google Scholar Cowan GR, Holtzman AH (1963) Flow configuration in colliding plates: explosive bonding. J Appl Phys 34:928–939Article ADS Google Scholar Christiansen EL (1995) Hypervelocity impact testing above 10 km/s of advanced orbital debris shields. In: Proceedings of APS conference on shock compression of condensed matter, pp 1183–1186 Google Scholar Mashimo T (1993) Shock waves in materials science. In: Sawaoka A (ed), Chap 6. Springer-Verlag, Tokyo, pp 113–144 Google Scholar Duvall GE, Graham

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RA (1977) Phase transitions under shock wave loading. Rev Mod Phys 43:523–579Article ADS Google Scholar Dlott DD (1995) Picosecond dynamics behind shock front. J Phys IV:C4, Suppl. III(5):C4-337-1-7 Google Scholar Noack J, Vogel A (1998) Single-shot spatially resolved characterization of laser-induced shock waves in water. Appl Opt 37:4092–4099Article ADS Google Scholar Nagayama K, Mori Y, Motegi Y, Nakahara M (2006) Shock Hugoniot for biological materials. Shock Waves 15:267–275Article ADS Google Scholar Nellis WJ, Moriarty JA, Mitchell AC, Ross M, Dandrea RG, Ashcroft NW, Holms NC, Gathers GR (1988) Metal physics at ultrahigh pressure: aluminum, copper, and lead as prototypes. Phys Rev Lett 60:1414–1417Article ADS Google Scholar Eliezer S, Ghatak A, Hora H (1986) An introduction to equation of state: theory and applications. Cambridge University Press Google Scholar Nagayama K (1994) New method of calculating shock temperature and entropy of solids based on the Hugoniot data. J Phys Soc Jpn 63:3737–3743Article ADS Google Scholar Chhabildas LC, Asay JR (1978) Rise-time measurements of shock transitions in aluminum, copper, and steel. J Appl Phys 50:2749–2754Article ADS Google Scholar Swegle JW, Grady DE (1985) Shock viscosity and the prediction of shock wave rise times. J Appl Phys 58:692–701Article ADS Google Scholar Rodean HC (1968) Relationship for condensed materials among heat of sublimation, shock-wave velocity, and particle velocity. J Chem Phys 49:4117–4127Article ADS Google Scholar Grüneisen E (1926) In: Greiger H, Scheel K (eds) Handbuch der Physik, 477, vol 10. Springer, Berlin, pp 1–59 Google Scholar Steinberg D (1981) The temperature independence of Grüneisen gamma. Download this free video of Wave Shock Flash from Pixabay's vast library of royalty-free stock images, videos and music. Wave shock flash free stock video. Free for use download. olenchic 3,785 Wave Shock Flash Explosion. Related free videos. HD 0:05. Shock Wave Flash. HD 0:05. Intro Wave Flash Light. HD 0:10. Shocking Outline Shock Thousands of stock shock wave videos to choose from. Free HD 4K video clips. Royalty-free videos. HD 0:05. Shock Wave Flash. HD 0:05. Wave Shock Flash. 4K 0:46. Wave Lighthouse

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NASA captures XB-1’s supersonic shockwave as it breaks the sound barrier US company Boom Supersonic collaborated with NASA to obtain specialized photographs of the supersonic test. Updated: Mar 04, 2025 09:02 AM ESTSchlieren photography was to capture and visualize the shock waves created by XB-1's supersonic flight.NASA/Boom Supersonic An XB-1 aircraft’s shock waves created during a supersonic flight have been captured using specialized ground-based photography. January saw XB-1 make history as the first privately developed civil supersonic aircraft to break the sound barrier in the United States.On February 10th, it achieved another successful supersonic flight. US company Boom Supersonic collaborated with NASA on the second flight to obtain specialized photographs of the supersonic test. A ground-based NASA team used Schlieren photography to capture and visualize the shock waves created by XB-1’s supersonic flight.NASA also gathered acoustic data from XB-1’s flight. Interestingly, the analysis showed that no sonic boom was audible on the ground during the supersonic flight.“This image makes the invisible visible—the first American-made civil supersonic jet breaking the sound barrier. Thanks to Geppetto’s [pilot] exceptional flying and our partnership with NASA, we were able to capture this iconic image,” said Blake Scholl, Founder and CEO of Boom Supersonic. “We also confirmed that XB-1 made no audible sonic boom, which paves the way for coast-to-coast flights up to 50% faster,” Scholl added. Perfect timing and position required Capturing the Schlieren images was a challenging feat, requiring perfect conditions, precise timing, and expert piloting. If successful, this technique reveals the invisible Scale called the diatomic scale which has 8 intervals (octave + 7 other intervals).→ Shock wave: It is defined as the wave produced by a body moving with a speed greater than the speed of sound. Shock waves carry a large amount of energy and when strike a building rattling sound due to the vibration of the building is produced.→ Mach number: It is defined as the ratio of the velocity of the body producing shock waves to the velocity of sound.∴ Mach number = \(\frac{\mathrm{V}_{\mathrm{s}}}{\mathrm{v}}\)→ Echo: It is defined as the repetition of the sound of short duration. It (echo) is heard if the minimum distance between the obstacle reflecting sound waves and the source of sound is 17 m.→ Reverberation: It is defined as the persistence or prolongation of audible sound after the source has stopped emitting sound. It is due to multiple reflections of sound waves.→ Reverberation time: It is defined as the time during which the intensity of sound falls to one million of its original value after the source has stopped producing it.→ The acoustics of Building: It is that branch of science which deals with the design of big halls and auditoriums so that a speech delivered or music produced in them is distinctly and clearly heard at all places in the building.Important Formulae:→ Velocity of wave: v = vλv = frequency of oscillator generating the waveλ = wavelength of the wavev = velocity of wave→ Velocity of transverse wave in a string:v = \(\sqrt{\frac{T}{m}}=\sqrt{\frac{T}{\pi r^{2} \rho}}\), whereρ = density of the material of stringr = radius of stringT = tension Applied on the stringm = mass per unit length of the string→ Newton’s form ula for velocity of sound in air:v = \(\sqrt{\frac{P}{\rho}}\)P = air pressureρ = density of air→ Velocity of elastic waves or longitudinal waves in a medium is:v = \(\sqrt{\frac{E}{\rho}}\)E = coefficient of elasticity of the mediumρ = density of the medium→ Leplace’s formula for velocity of sound is air/gases:v = \(\sqrt{\frac{\gamma \mathrm{P}}{\rho}}\) whereE = γP = adiabatic elasticity of air/gasρ = density of air/gasγ = CP/CV.→ Velocity of wave in gas/liquid medium (Longitudinal wave):V = \(\sqrt{\frac{Y}{\rho}}\), whereY = Young’s modulusρ = coefficient of rigidity→ Velocity as a function of:1. temperature, \(\frac{v_{1}}{v_{2}}=\sqrt{\frac{T_{1}}{T_{2}}}\)2. density, \(\frac{v_{1}}{v_{2}}=\sqrt{\frac{\rho_{1}}{\rho_{2}}}\)→ The equation of a plane simple harmonic wave (progressive wave) travelling from left to right is:y = A sin 2π(\(\frac{\mathrm{t}}{\mathrm{T}}-\frac{\mathrm{x}}{\lambda}\))= A sin \(\frac{2 \pi}{\lambda}\)(vt – x)= A sin (ωt – kx)and from right to left i.e. along – X axis is obtained by replacingx = -x, i.e. y = A sin \(\frac{2 \pi}{\lambda}\)(vt – x)→ Phase difference = \(\frac{2 \pi}{\lambda}\) × path differenceorΔΦ = \(\frac{2 \pi}{\lambda}\) × Δx→ Total energy transmitted per Unit volume in waves

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When you purchase through links on our site, we may earn an affiliate commissionDynamics Calculators overviewDynamics Calculators comprises a selection of 5 different calculators that will simplify calculations which have given you headaches so far. Complex calculations, such as Oscillation Period of Double Pendulum, Mach Wedge Angle for Shock Waves, and others listed below will be handled easily with this app. Young Modulus of Isotropic Elastic Solids Terminal Velocity Impedance of Forced Oscillations Oscillation Period of Double Pendulum Mach Wedge Angle for Shock Waves Features Formula and description for each calculator Copy / Paste params and results Clean, simple and easy to use What’s new in version 1.1Version 1.1: Bug fixes and stability improvements Write your thoughts in our old-fashioned commentMacUpdate Comment Policy. We strongly recommend leaving comments, however comments with abusive words, bullying, personal attacks of any type will be moderated.Email me when someone replies to this comment(0 Reviews of Dynamics Calculators)There are no reviews yetCommentsUser RatingsHelp the communityThere are no reviews yet, be the first to leave oneHelp the communityThere are no ratings yet, be the first to leave oneHow would you rate Dynamics Calculators?

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Different components of your plumbing and pumping systems. That’s why it’s important to get rid of water hammer as soon as possible. A loose pipe or worn stop value could end up costing you thousands of pounds.Secure Any Loose PipesIf loose pipes are turning mild shock waves into loud bangs, you can prevent it by securing pipe straps, adding new pipe straps or tightening studs or joists.Remember, do not mix different metals when securing pipes. A steel strap should not be used to secure a copper pipe or vice versa. Different metals can chemically react and cause corrosion of the metal.If the problem pipes are located in hidden areas, then you will more than likely need a plumber to come out and help you find the issue.Wrap Pipes in Foam InsulationAnother idea is to wrap pipes in foam insulation. The foam should help prevent banging by absorbing the shock waves. This can also help prevent pipes from freezing in the winter. Make sure to leave space for expansion around the pipe.Fix Washing Machines or DishwashersIf the banging only occurs when using the washing machine or dishwasher, then the problem is likely the solenoid valve. The solenoid valve is a component of your machine used to shut off the water supply. If the response time of the solenoid valve is too quick, then the fluid inside the valve is abruptly stopped. In this case, the fluid reflects like a wave causing a shock wave back up the pipe that you hear as a bang. The simple fix is to choose a solenoid valve or other valve type that has a slower response time.Install a Water-Pressure RegulatorA common cause of water hammer is high water pressure. If your pressure is running near 100 psi, then it’s likely the cause of your issue.. Download this free video of Wave Shock Flash from Pixabay's vast library of royalty-free stock images, videos and music. Wave shock flash free stock video. Free for use download. olenchic 3,785 Wave Shock Flash Explosion. Related free videos. HD 0:05. Shock Wave Flash. HD 0:05. Intro Wave Flash Light. HD 0:10. Shocking Outline Shock

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Helps prevent progression to Type III block. Remmebr that 3 degree block is a random, no relationship at all btw A and V beating on EKG. Acute MI management: FSOM include O2, IV access and give aspirin and nitro. ACEI aren’t used acutely but reduces mortality if taken for the weeks after an MI. bb helps w/ decrease myocardial demand and controls HR. Can give after aspirin, nitro, and morphine. Acute MI: If EKG shows ST segment elevation in 2 contiguous leads, then thrombolytics are indicated, and if pt presents within 12-24 h of symptoms. Must give NO before getting the EKG. Contra for thrombolytics are active bleed, any intracranial event (bleed, ischemia, neoplasm), SBP > 180, or trauma. Don’t confuse with ST segment depression, which is just ischemia. Flash pulmonary edema: Presents w/ acute onset of SOB. No previous history necessary. Hypertensive crisis can cause it, so look for a very high BP. CXR looks like lots of edema, and there willl be diffuse crackles. FSOM in any flash pul edema is give O2 (O2 sat will be low), morphine, and IV furosemide (loop diuretics). If the cause is HTN crisis, the preferred drug to give is IV NO or nitroprusside. Other causes of flash pul edema: mitral stenosis or acute aortic/mitral regurg. Thus, after someone has an episode of this, get an echo. Bb are CONTRAINDICATED in acute heart failure, can slow heart too much and lead to death. Cardiogenic pulmonary edema: Initial Rx is similar: O2, morphine (reduces work of breathing), and a loop diuretic. Cardiogenic shock complicated by hypotension: dopamine is a good choice. Acute pericarditis: can be infarct associated, and happen after an MI (esp. transmural). The associated CP depends on position, and worsens w/ deep inspiration. EKG has diffuse ST elevation w/ PR depression. Rub is heard voer L sternal border (a scratchy sound), which gets louder as pt leans forward. Rx is NSAIDS (or anything for pain). Dressler’s syndrome: happens in MI pt and after cardiac surgery. Usually develops weeks/months after MI not days. Presents w/ fever, leukocytosis, pleuritic chest pain, and pericardial rub. Thus, very similar to pericarditis, but look at the time course. Q waves are indicative of old infarct (days old sometimes) Aortic stenosis: Area of aortic valve Syncope w/o any apparent cause is most likely neurocardiogenic. Prodrome of nausea, lightheadedness, pallor, and diaphoresis. Precipitating events include prolonged standing, exertion,