Your not phatho youweigh sooo much more than phat your souvh bigger than phatso Great f****** run
@joshmcdonaldcomic6 ай бұрын
How did you add elevator to the sky
@samzstd337 ай бұрын
Who's doing these videos thank you you're doing a good job
@supertreeofficial7 ай бұрын
Thank you
@samzstd337 ай бұрын
Who me?
@samzstd338 ай бұрын
wire me out
@Rywkek8 ай бұрын
❤❤❤❤❤
@Катюха-б3ю9 ай бұрын
Спасибо брат 💃💃💃💃💃💃💃
@SunorTroub9 ай бұрын
Dud, I made this💀, gimmie the credits please
@supertreeofficial7 ай бұрын
I didn't get this from you
@SunorTroub7 ай бұрын
Dude, you got it, right here 0:17 there's a problem separating the audio I made
@SunorTroub7 ай бұрын
kzbin.info/www/bejne/iYLOp2h4jNB8jJosi=4_JGcyQwrlwbNSae It's the same audio separation error as this video
@gladispalomino715310 ай бұрын
De donde sacaste la foto de Turbo junto a Cornelius Cummigns 😮?
@supertreeofficial7 ай бұрын
On Oliver's instagram idk if it's still up though
@supertreeofficial11 ай бұрын
Join my discord server discord.com/invite/pR63Rdxa
@DollarsRecordsOfficial Жыл бұрын
dope
@OliverTreeLeakedMe_Official Жыл бұрын
First (sorry kids)
@whatbank6797 Жыл бұрын
I fw it shits nice as usual oliver keep it up
@CoNtAiNeR93 Жыл бұрын
Ah damn its half past 11 and im pissed..yeah it's a weekday..im the invisible man🏈
@militarygecko78 Жыл бұрын
yay
@user-uy5py5ih2t Жыл бұрын
Lol this is actually really good. Nice job!
@brett-o3i Жыл бұрын
Whoa this needs to be more widely spread
@MrRussotv Жыл бұрын
Can I get my 2 minuets and 38 seconds back?
@supertreeofficial Жыл бұрын
Nope, you chose to watch the video so that's on you 😉
@feelincrispy7053 Жыл бұрын
What in the hell was that
@supertreeofficial Жыл бұрын
???
@stoleprodigy Жыл бұрын
Oliver Grandpa.
@chadruland5460 Жыл бұрын
WWEEEEEEEEEEEEEEEEEEE
@chadruland5460 Жыл бұрын
Love me some Oliver tree!
@sorasnowfall Жыл бұрын
This is good
@Mrvuaetex Жыл бұрын
Epic
@jaarva_ Жыл бұрын
it's not the demo, it's just a fanmade version
@supertreeofficial Жыл бұрын
It's a remake of the live version
@pairpunchgaming1394 Жыл бұрын
In physics, quantum tunnelling, barrier penetration, or simply tunnelling is a quantum mechanical phenomenon in which an object such as an electron or atom passes through a potential energy barrier that, according to classical mechanics, the object does not have sufficient energy to enter or surmount. Tunneling is a consequence of the wave nature of matter, where the quantum wave function describes the state of a particle or other physical system, and wave equations such as the Schrödinger equation describe their behavior. The probability of transmission of a wave packet through a barrier decreases exponentially with the barrier height, the barrier width, and the tunneling particle's mass, so tunneling is seen most prominently in low-mass particles such as electrons or protons tunneling through microscopically narrow barriers. Tunneling is readily detectable with barriers of thickness about 1-3 nm or smaller for electrons, and about 0.1 nm or smaller for heavier particles such as protons or hydrogen atoms.[1] Some sources describe the mere penetration of a wave function into the barrier, without transmission on the other side, as a tunneling effect, such as in tunneling into the walls of a finite potential well.[2][3] Tunneling plays an essential role in physical phenomena such as nuclear fusion[4] and alpha radioactive decay of atomic nuclei. Tunneling applications include the tunnel diode,[5] quantum computing, flash memory, and the scanning tunneling microscope. Tunneling limits the minimum size of devices used in microelectronics because electrons tunnel readily through insulating layers and transistors that are thinner than about 1 nm.[6][7] The effect was predicted in the early 20th century. Its acceptance as a general physical phenomenon came mid-century.[8] Introduction to the concept 1:31CC Animation showing the tunnel effect and its application to an STM Quantum tunnelling falls under the domain of quantum mechanics: the study of what happens at the quantum scale. Tunnelling cannot be directly perceived. Much of its understanding is shaped by the microscopic world, which classical mechanics cannot explain. To understand the phenomenon, particles attempting to travel across a potential barrier can be compared to a ball trying to roll over a hill. Quantum mechanics and classical mechanics differ in their treatment of this scenario. Classical mechanics predicts that particles that do not have enough energy to classically surmount a barrier cannot reach the other side. Thus, a ball without sufficient energy to surmount the hill would roll back down. In quantum mechanics, a particle can, with a small probability, tunnel to the other side, thus crossing the barrier. This tunnelling leaves the barrier unaffected (i.e. no hole is created in the barrier). The reason for this difference comes from treating matter as having properties of waves and particles. One interpretation of this duality involves the Heisenberg uncertainty principle, which defines a limit on how precisely the position and the momentum of a particle can be simultaneously known.[9] This implies that no solutions have a probability of exactly zero (or one), though it may approach infinity. If, for example, the calculation for its position was taken as a probability of 1, its speed would have to be infinity (an impossibility). Hence, the probability of a given particle's existence on the opposite side of an intervening barrier is non-zero, and such particles will appear on the 'other' (a semantically difficult word in this instance) side in proportion to this probability. The tunnelling problem A simulation of a wave packet incident on a potential barrier. In relative units, the barrier energy is 20, greater than the mean wave packet energy of 14. A portion of the wave packet passes through the barrier. The wave function of a physical system of particles specifies everything that can be known about the system.[10] Therefore, problems in quantum mechanics analyze the system's wave function. Using mathematical formulations, such as the Schrödinger equation, the time evolution of a known wave function can be deduced. The square of the absolute value of this wave function is directly related to the probability distribution of the particle positions, which describes the probability that the particles would be measured at those positions. As shown in the animation, a wave packet impinges on the barrier, most of it is reflected and some is transmitted through the barrier. The wave packet becomes more de-localized: it is now on both sides of the barrier and lower in maximum amplitude, but equal in integrated square-magnitude, meaning that the probability the particle is somewhere remains unity. The wider the barrier and the higher the barrier energy, the lower the probability of tunneling. Some models of a tunneling barrier, such as the rectangular barriers shown, can be analysed and solved algebraically.[11]: 96 Most problems do not have an algebraic solution, so numerical solutions are used. "Semiclassical methods" offer approximate solutions that are easier to compute, such as the WKB approximation.
@supertreeofficial Жыл бұрын
Respect for writing this, but I ain't readin all dat