"More like 12 years of Christmas!" xD One of my favorite parts. Well, except the last part. lol Totally something my sister would say. "Let's not and say we did!"
I guess Im asking the wrong place but does any of you know a way to get back into an Instagram account?? I somehow forgot the account password. I appreciate any tips you can give me!
wonder if i listen to this song too much when i sing it every second hour everytime i have a smoke O.o or i might sing the scrubs version sometimes too xD
In the mathematically rigorous formulation of quantum mechanics developed by Paul Dirac,[13] David Hilbert,[14] John von Neumann,[15] and Hermann Weyl[16] the possible states of a quantum mechanical system are represented by unit vectors (called "state vectors"). Formally, these reside in a complex separable Hilbert space - variously called the "state space" or the "associated Hilbert space" of the system - that is well defined up to a complex number of norm 1 (the phase factor). In other words, the possible states are points in the projective space of a Hilbert space, usually called the complex projective space. The exact nature of this Hilbert space is dependent on the system - for example, the state space for position and momentum states is the space of square-integrable functions, while the state space for the spin of a single proton is just the product of two complex planes. Each observable is represented by a maximally Hermitian (precisely: by a self-adjoint) linear operator acting on the state space. Each eigenstate of an observable corresponds to an eigenvector of the operator, and the associated eigenvalue corresponds to the value of the observable in that eigenstate. If the operator's spectrum is discrete, the observable can attain only those discrete eigenvalues. In the formalism of quantum mechanics, the state of a system at a given time is described by a complex wave function, also referred to as state vector in a complex vector space.[17] This abstract mathematical object allows for the calculation of probabilities of outcomes of concrete experiments. For example, it allows one to compute the probability of finding an electron in a particular region around the nucleus at a particular time. Contrary to classical mechanics, one can never make simultaneous predictions of conjugate variables, such as position and momentum, with accuracy. For instance, electrons may be considered (to a certain probability) to be located somewhere within a given region of space, but with their exact positions unknown. Contours of constant probability, often referred to as "clouds", may be drawn around the nucleus of an atom to conceptualize where the electron might be located with the most probability. Heisenberg's uncertainty principle quantifies the inability to precisely locate the particle given its conjugate momentum.[18] According to one interpretation, as the result of a measurement the wave function containing the probability information for a system collapses from a given initial state to a particular eigenstate. The possible results of a measurement are the eigenvalues of the operator representing the observable - which explains the choice of Hermitian operators, for which all the eigenvalues are real. The probability distribution of an observable in a given state can be found by computing the spectral decomposition of the corresponding operator. Heisenberg's uncertainty principle is represented by the statement that the operators corresponding to certain observables do not commute. The probabilistic nature of quantum mechanics thus stems from the act of measurement. This is one of the most difficult aspects of quantum systems to understand. It was the central topic in the famous Bohr-Einstein debates, in which the two scientists attempted to clarify these fundamental principles by way of thought experiments. In the decades after the formulation of quantum mechanics, the question of what constitutes a "measurement" has been extensively studied. Newer interpretations of quantum mechanics have been formulated that do away with the concept of "wavefunction collapse" (see, for example, the relative state interpretation). The basic idea is that when a quantum system interacts with a measuring apparatus, their respective wavefunctions become entangled, so that the original quantum system ceases to exist as an independent entity. For details, see the article on measurement in quantum mechanics.[19] Generally, quantum mechanics does not assign definite values. Instead, it makes a prediction using a probability distribution; that is, it describes the probability of obtaining the possible outcomes from measuring an observable. Often these results are skewed by many causes, such as dense probability clouds. Probability clouds are approximate, but better than the Bohr model, whereby electron location is given by a probability function, the wave function eigenvalue, such that the probability is the squared modulus of the complex amplitude, or quantum state nuclear attraction.[20][21] Naturally, these probabilities will depend on the quantum state at the "instant" of the measurement. Hence, uncertainty is involved in the value. There are, however, certain states that are associated with a definite value of a particular observable. These are known as eigenstates of the observable ("eigen" can be translated from German as meaning "inherent" or "characteristic").[22] In the everyday world, it is natural and intuitive to think of everything (every observable) as being in an eigenstate. Everything appears to have a definite position, a definite momentum, a definite energy, and a definite time of occurrence. However, quantum mechanics does not pinpoint the exact values of a particle's position and momentum (since they are conjugate pairs) or its energy and time (since they too are conjugate pairs); rather, it provides only a range of probabilities in which that particle might be given its momentum and momentum probability. Therefore, it is helpful to use different words to describe states having uncertain values and states having definite values (eigenstates). Usually, a system will not be in an eigenstate of the observable (particle) we are interested in. However, if one measures the observable, the wavefunction will instantaneously be an eigenstate (or "generalized" eigenstate) of that observable. This process is known as wavefunction collapse, a controversial and much-debated process[23] that involves expanding the system under study to include the measurement device. If one knows the corresponding wave function at the instant before the measurement, one will be able to compute the probability of the wavefunction collapsing into each of the possible eigenstates. For example, the free particle in the previous example will usually have a wavefunction that is a wave packet centered around some mean position x0 (neither an eigenstate of position nor of momentum). When one measures the position of the particle, it is impossible to predict with certainty the result.[19] It is probable, but not certain, that it will be near x0, where the amplitude of the wave function is large. After the measurement is performed, having obtained some result x, the wave function collapses into a position eigenstate centered at x.[24] The time evolution of a quantum state is described by the Schrödinger equation, in which the Hamiltonian (the operator corresponding to the total energy of the system) generates the time evolution. The time evolution of wave functions is deterministic in the sense that - given a wavefunction at an initial time - it makes a definite prediction of what the wavefunction will be at any later time.[25] During a measurement, on the other hand, the change of the initial wavefunction into another, later wavefunction is not deterministic, it is unpredictable (i.e., random). A time-evolution simulation can be seen here.[26][27] Wave functions change as time progresses. The Schrödinger equation describes how wavefunctions change in time, playing a role similar to Newton's second law in classical mechanics. The Schrödinger equation, applied to the aforementioned example of the free particle, predicts that the center of a wave packet will move through space at a constant velocity (like a classical particle with no forces acting on it). However, the wave packet will also spread out as time progresses, which means that the position becomes more uncertain with time. This also has the effect of turning a position eigenstate (which can be thought of as an infinitely sharp wave packet) into a broadened wave packet that no longer represents a (definite, certain) position eigenstate.[28] Fig. 1: Probability densities corresponding to the wavefunctions of an electron in a hydrogen atom possessing definite energy levels (increasing from the top of the image to the bottom: n = 1, 2, 3, ...) and angular momenta (increasing across from left to right: s, p, d, ...). Brighter areas correspond to higher probability density in a position measurement. Such wavefunctions are directly comparable to Chladni's figures of acoustic modes of vibration in classical physics, and are modes of oscillation as well, possessing a sharp energy and, thus, a definite frequency. The angular momentum and energy are quantized, and take only discrete values like those shown (as is the case for resonant frequencies in acoustics) Some wave functions produce probability distributions that are constant, or independent of time - such as when in a stationary state of constant energy, time vanishes in the absolute square of the wave function. Many systems that are treated dynamically in classical mechanics are described by such "static" wave functions. For example, a single electron in an unexcited atom is pictured classically as a particle moving in a circular trajectory around the atomic nucleus, whereas in quantum mechanics it is described by a static, spherically symmetric wavefunction surrounding the nucleus (Fig. 1) (note, however, that only the lowest angular momentum states, labeled s, are spherically symmetric).[29] The Schrödinger equation acts on the entire probability amplitude, not merely its absolute value. Whereas the absolute value of the probability amplitude encodes information about probabilities, its phase encodes information about the interference between quantum states. This gives rise to the "wave-like" behavior of quantum states. As it turns out, analytic solutions of the Schrödinger equation are available for only a very small number of relatively simple model Hamiltonians, of which the quantum harmonic oscillator, the particle in a box, the hydrogen molecular ion, and the hydrogen atom are the most important representatives. Even the helium atom - which contains just one more electron than does the hydrogen atom - has defied all attempts at a fully analytic treatment. There exist several techniques for generating approximate solutions, however. In the important method known as perturbation theory, one uses the analytic result for a simple quantum mechanical model to generate a result for a more complicated model that is related to the simpler model by (for one example) the addition of a weak potential energy. Another method is the "semi-classical equation of motion" approach, which applies to systems for which quantum mechanics produces only weak (small) deviations from classical behavior. These deviations can then be computed based on the classical motion. This approach is particularly important in the field of quantum chaos.
1. Yeah! 2. Heavenly creatures! 3. Ya ya ya! 4. Aah! *BOOM* 5. Let me guess... Five onion rings! I knew it! 6. You brake it, you bought it. 7. *Guitar riff* 8. Don't you dare! 9. Oh oh! I'm sorry, Gordo! 10. No strings attached! 11. *Fairies tingling* 12. Da da da da da da!
12 beaten children 11 drive by shootings 10 frozen homeless 9 amputations 8 burned victims 7 strangled shoppers 6 random knifings 5 suicides 4 beaten wives 3 ODs 2 shattered skulls and a drunk who drove into a tree this is my favorite version
@wizard101Gamezhere1 7) 3:00 ''Eleven fairies dusting'' (Not ''fairys'') + On ''the'' 11th Day 8) 1:38 From there it says: On the seventh day of Christmas my true love gave to me seven sorts of jelly. And ONLY on the 12th day of Christmas it is "Seven dwarfs a jamming'' . 9) The TITLE of the song. It's CHRISTMAS (Not "Chirstmas") And there were several other tiny mistakes which I didn't mention.
I used to have the Shrek Christmas CD and this was my absolute favorite song on the CD. Listened to it everyday until Christmas when I first got it.
zero granger stop that
Me too
At school we sing two Christmas song and this is one our whole class knows this song
10 years later I still jam to this song every year.
i just stayed silent till the 5th day of christmas.....
Same
I love this song
Shrek: More like the 12 years of Christmas!
Shrek, I don't blame you! Considering how long this song seemed to go on despite being 4 minutes long!
Chorus: 2 weed rats!
Gingy: HEAVENLY CREATURES!!!
Chorus: 8 cookies dunking!
Gingy: DON'T YOU DARE!
I love that part!
I am always looking forward to CHRISTMAS and not just the gifts, but also the warmth and love and joy of family all around celebrating Jesus's b-day
"More like 12 years of Christmas!" xD One of my favorite parts. Well, except the last part. lol Totally something my sister would say. "Let's not and say we did!"
I guess Im asking the wrong place but does any of you know a way to get back into an Instagram account??
I somehow forgot the account password. I appreciate any tips you can give me!
@Salvador Alessandro Instablaster =)
Love both those parts! Too funny! XD
1st Day: The Spinosaurus just for me
2nd Day: 2 Fluffy Tyrannosauruses
3rd Day: 3 Brachiosauruses eating
4th Day: 4 Singing Parasaurolophuses
5th Day: 5 Golden Kulindadromeuses
6th Day: 6 Raptors Playing
7th Day: 7 Triceratopses Herding
8th Day: 8 Stegosaurus Flushing
9th Day: 9 Ankylosaurs Hobbling
10th Day: 10 Ornithopods Running
11th Day: 11 Pachycephalosaurs fighting
12th Day: 12 Allosauruses still Living
Oh man I haven't heard this in years. I only heard it once on the bus coming home from school on a CD this song was genius.
I ran out of breath trying to sing that.
This version rocks!!
i like this version
Me too
My bus driver used to play this cd for us on the week before christmas. This is so nostalgic 🥹
That song reminds me that time at my elementary school Christmas concert I was dancing with Shrek
wonder if i listen to this song too much when i sing it every second hour everytime i have a smoke O.o or i might sing the scrubs version sometimes too xD
I listen to this every christmas it never gets old
Every Christmas I'll ever go back here and sing this song
lol "more like the 12 years of Christmas" lol i love sherk its one of my fav movies lol good work
That was way better than the real 12 days of Christmas
We did this for school one year, so fun. I got to hold the puppets sign, so fun :)
lmao XD
donkey: lets do that again!
shrek: lets not and say we did xD thats so funny XD
In the mathematically rigorous formulation of quantum mechanics developed by Paul Dirac,[13] David Hilbert,[14] John von Neumann,[15] and Hermann Weyl[16] the possible states of a quantum mechanical system are represented by unit vectors (called "state vectors"). Formally, these reside in a complex separable Hilbert space - variously called the "state space" or the "associated Hilbert space" of the system - that is well defined up to a complex number of norm 1 (the phase factor). In other words, the possible states are points in the projective space of a Hilbert space, usually called the complex projective space. The exact nature of this Hilbert space is dependent on the system - for example, the state space for position and momentum states is the space of square-integrable functions, while the state space for the spin of a single proton is just the product of two complex planes. Each observable is represented by a maximally Hermitian (precisely: by a self-adjoint) linear operator acting on the state space. Each eigenstate of an observable corresponds to an eigenvector of the operator, and the associated eigenvalue corresponds to the value of the observable in that eigenstate. If the operator's spectrum is discrete, the observable can attain only those discrete eigenvalues.
In the formalism of quantum mechanics, the state of a system at a given time is described by a complex wave function, also referred to as state vector in a complex vector space.[17] This abstract mathematical object allows for the calculation of probabilities of outcomes of concrete experiments. For example, it allows one to compute the probability of finding an electron in a particular region around the nucleus at a particular time. Contrary to classical mechanics, one can never make simultaneous predictions of conjugate variables, such as position and momentum, with accuracy. For instance, electrons may be considered (to a certain probability) to be located somewhere within a given region of space, but with their exact positions unknown. Contours of constant probability, often referred to as "clouds", may be drawn around the nucleus of an atom to conceptualize where the electron might be located with the most probability. Heisenberg's uncertainty principle quantifies the inability to precisely locate the particle given its conjugate momentum.[18]
According to one interpretation, as the result of a measurement the wave function containing the probability information for a system collapses from a given initial state to a particular eigenstate. The possible results of a measurement are the eigenvalues of the operator representing the observable - which explains the choice of Hermitian operators, for which all the eigenvalues are real. The probability distribution of an observable in a given state can be found by computing the spectral decomposition of the corresponding operator. Heisenberg's uncertainty principle is represented by the statement that the operators corresponding to certain observables do not commute.
The probabilistic nature of quantum mechanics thus stems from the act of measurement. This is one of the most difficult aspects of quantum systems to understand. It was the central topic in the famous Bohr-Einstein debates, in which the two scientists attempted to clarify these fundamental principles by way of thought experiments. In the decades after the formulation of quantum mechanics, the question of what constitutes a "measurement" has been extensively studied. Newer interpretations of quantum mechanics have been formulated that do away with the concept of "wavefunction collapse" (see, for example, the relative state interpretation). The basic idea is that when a quantum system interacts with a measuring apparatus, their respective wavefunctions become entangled, so that the original quantum system ceases to exist as an independent entity. For details, see the article on measurement in quantum mechanics.[19]
Generally, quantum mechanics does not assign definite values. Instead, it makes a prediction using a probability distribution; that is, it describes the probability of obtaining the possible outcomes from measuring an observable. Often these results are skewed by many causes, such as dense probability clouds. Probability clouds are approximate, but better than the Bohr model, whereby electron location is given by a probability function, the wave function eigenvalue, such that the probability is the squared modulus of the complex amplitude, or quantum state nuclear attraction.[20][21] Naturally, these probabilities will depend on the quantum state at the "instant" of the measurement. Hence, uncertainty is involved in the value. There are, however, certain states that are associated with a definite value of a particular observable. These are known as eigenstates of the observable ("eigen" can be translated from German as meaning "inherent" or "characteristic").[22]
In the everyday world, it is natural and intuitive to think of everything (every observable) as being in an eigenstate. Everything appears to have a definite position, a definite momentum, a definite energy, and a definite time of occurrence. However, quantum mechanics does not pinpoint the exact values of a particle's position and momentum (since they are conjugate pairs) or its energy and time (since they too are conjugate pairs); rather, it provides only a range of probabilities in which that particle might be given its momentum and momentum probability. Therefore, it is helpful to use different words to describe states having uncertain values and states having definite values (eigenstates). Usually, a system will not be in an eigenstate of the observable (particle) we are interested in. However, if one measures the observable, the wavefunction will instantaneously be an eigenstate (or "generalized" eigenstate) of that observable. This process is known as wavefunction collapse, a controversial and much-debated process[23] that involves expanding the system under study to include the measurement device. If one knows the corresponding wave function at the instant before the measurement, one will be able to compute the probability of the wavefunction collapsing into each of the possible eigenstates. For example, the free particle in the previous example will usually have a wavefunction that is a wave packet centered around some mean position x0 (neither an eigenstate of position nor of momentum). When one measures the position of the particle, it is impossible to predict with certainty the result.[19] It is probable, but not certain, that it will be near x0, where the amplitude of the wave function is large. After the measurement is performed, having obtained some result x, the wave function collapses into a position eigenstate centered at x.[24]
The time evolution of a quantum state is described by the Schrödinger equation, in which the Hamiltonian (the operator corresponding to the total energy of the system) generates the time evolution. The time evolution of wave functions is deterministic in the sense that - given a wavefunction at an initial time - it makes a definite prediction of what the wavefunction will be at any later time.[25]
During a measurement, on the other hand, the change of the initial wavefunction into another, later wavefunction is not deterministic, it is unpredictable (i.e., random). A time-evolution simulation can be seen here.[26][27]
Wave functions change as time progresses. The Schrödinger equation describes how wavefunctions change in time, playing a role similar to Newton's second law in classical mechanics. The Schrödinger equation, applied to the aforementioned example of the free particle, predicts that the center of a wave packet will move through space at a constant velocity (like a classical particle with no forces acting on it). However, the wave packet will also spread out as time progresses, which means that the position becomes more uncertain with time. This also has the effect of turning a position eigenstate (which can be thought of as an infinitely sharp wave packet) into a broadened wave packet that no longer represents a (definite, certain) position eigenstate.[28]
Fig. 1: Probability densities corresponding to the wavefunctions of an electron in a hydrogen atom possessing definite energy levels (increasing from the top of the image to the bottom: n = 1, 2, 3, ...) and angular momenta (increasing across from left to right: s, p, d, ...). Brighter areas correspond to higher probability density in a position measurement. Such wavefunctions are directly comparable to Chladni's figures of acoustic modes of vibration in classical physics, and are modes of oscillation as well, possessing a sharp energy and, thus, a definite frequency. The angular momentum and energy are quantized, and take only discrete values like those shown (as is the case for resonant frequencies in acoustics)
Some wave functions produce probability distributions that are constant, or independent of time - such as when in a stationary state of constant energy, time vanishes in the absolute square of the wave function. Many systems that are treated dynamically in classical mechanics are described by such "static" wave functions. For example, a single electron in an unexcited atom is pictured classically as a particle moving in a circular trajectory around the atomic nucleus, whereas in quantum mechanics it is described by a static, spherically symmetric wavefunction surrounding the nucleus (Fig. 1) (note, however, that only the lowest angular momentum states, labeled s, are spherically symmetric).[29]
The Schrödinger equation acts on the entire probability amplitude, not merely its absolute value. Whereas the absolute value of the probability amplitude encodes information about probabilities, its phase encodes information about the interference between quantum states. This gives rise to the "wave-like" behavior of quantum states. As it turns out, analytic solutions of the Schrödinger equation are available for only a very small number of relatively simple model Hamiltonians, of which the quantum harmonic oscillator, the particle in a box, the hydrogen molecular ion, and the hydrogen atom are the most important representatives. Even the helium atom - which contains just one more electron than does the hydrogen atom - has defied all attempts at a fully analytic treatment.
There exist several techniques for generating approximate solutions, however. In the important method known as perturbation theory, one uses the analytic result for a simple quantum mechanical model to generate a result for a more complicated model that is related to the simpler model by (for one example) the addition of a weak potential energy. Another method is the "semi-classical equation of motion" approach, which applies to systems for which quantum mechanics produces only weak (small) deviations from classical behavior. These deviations can then be computed based on the classical motion. This approach is particularly important in the field of quantum chaos.
i remember hearirng this in 2nd grade...loved all the songs from shrek
Fav christmas song EVER.
listen to this every year
this is so much better that the partridge in a pear tree version
8 more days and it's the 6 year anniversary of this awesome video.
I think I memorized this a lot more than my notes for Music.
This is so awesome ! ;)
A great example to use for my English class - students can come up with their own lyrics. Thanks and Merry Christmas 2012!
well 8888gummybear I am listening to this a week before thanksgiving and i'll give you a thumbs up:)
Great Stuff
I needed something to cheer me up. this worked,
thank you
this version is fun and so cool! :-D
It’s that time of the years boys
Love it, that 5 Onion Rings is sang so epic anytime :D
awesome i love this i listen to this everyday on my ipod thx for putting this on yt
12 years of Christmas lol! This is really funny!
I'm head over heels in love with this song
this was awesome!!!!!!! i luv donkey n shrek their amazing!!!!! ;)
thisis so funny keep doing this veido on christmas it should be a popular.
that was the best xmas song ive ever herad!!!
i absulutley love it
cant wait until christmas I like the song
this was excellent
Would you prefer this or The Phineas and Ferb version?
lmao shrek and them crew made an awsome christmas song
1 OF THE BEST SONGS I HEARD EVER
i absolutely luvd it:)
5 onion rings, 4 toilet bowls,3 french fries,2 ca sa bao,and a ah bei on a pear tree
Omg this so so f*cking funny and I have absolutley NO COMPLAINTS you rock BloodShrinkiro
TEN PUPPETS DANCING! " NO STRINGS ATTACHED" LOL LOVE THIS SONG :D
i really miss this song in in yr 8 and i heard this song when i was in yr3 or yr2
omg this is great this is an awsome version!!!
best christmas song ever LLLLLOOOOOLLLLL
1. Yeah!
2. Heavenly creatures!
3. Ya ya ya!
4. Aah! *BOOM*
5. Let me guess... Five onion rings! I knew it!
6. You brake it, you bought it.
7. *Guitar riff*
8. Don't you dare!
9. Oh oh! I'm sorry, Gordo!
10. No strings attached!
11. *Fairies tingling*
12. Da da da da da da!
I'm watching this on the last day on November ^^
love it love it love it... a lot better then that other mess
Brilliant song love it
THe BEST SONG I HAVE EVER HERD
OMG !!!! I LUV THIS SONG ITS SO FUNNAH YA YA YA YA !!!!!! WELL DONE BLOODSHINKIRO !!!!
Absolute Banger!
very funny, i love this song!!!!
"9 nice mine a tripping" hahaha!
love this song
Great ho ho ho Merry Chirstmas
lol and my fire breather dragon, 5 onion ring 7 dwarms jamming. lol
I always thought it was a "Fire Breathing Dragon Dress."
Best one yet!!~
this is awesome
LOL sweet dude.lets listen to that again!!
I always crack up at the 5 ONION RINGS!
this is from the limited edition christmas version shrek soundtrack
love dis!!
hahahah oh god this is awesome...wait Donkey is hilarious and this is a epic version of it
i Like It (: Ihhts One Of My Best Song This Chrismas I Also Listen To It In The Shower (x
we sang this in elementary school, i loved my english teacher
Beatiful song i Study this song in my class and Merry Cristmas:> :) 🌲
Damn Dude I was Drinking Sprite and I Almost Spit it on my Laptop. Nice Song.
I luv this!!!!!!!!!! it's the best version ever, it's soooooooooooooooooooooooooooooo funny!!!!!!!!!!!!!!!!!! :)
i started cracking up laughing hahah thanks nice vid!
when i saw this the first time i laughed at the whole thing...very funny video
i love this!!!!!!!! i never heard it before! 5 onionnnnnn rinnggggsssss LOL
I am gonna sing this to my family on Christmas! HA HA HA!
12 beaten children
11 drive by shootings
10 frozen homeless
9 amputations
8 burned victims
7 strangled shoppers
6 random knifings
5 suicides
4 beaten wives
3 ODs
2 shattered skulls
and a drunk who drove into a tree
this is my favorite version
Awsome i love it!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!
Best song ever
Fiffeeee Oniooooooooon riiiiiiiiiings :D haha We always singing this on English lesson xD
Galileo tripped while being afraid of mayonnaise at yoga class in 2009
i like this song moor than the regular 12 days of christmas.
1-They are changeing the tonality each time since the fourth day. C, DbM, D, EbM, etc.
2- 2:55 ¿ya volví? (I came back)
Absolutely loved it hehehe so very funny!
I love all things shrek an christmas so to get the 2 together brill :D:D
sooo jolly
i love that!
i love this version!!! its so funny i love shrek!! LOL>_
cute i love it! :D
i love this song amazing
12 day: 12 pokemon singing
11 day: 11 pies a baking
10 day: 10 bars of chocolate
9 day: 9 snowflakes falling
8 day: 8 puppets talkative
7 day: 7 the doraemons
6 day: 6 Twilight's friends
5 day: 5 kamaboko sleeping
4 day: 4 alicorns
3: 3 ghosts a scaring
2: best friends
And a fairy that made a fantastic wink.
most epic christmas song ever!!
i also noticed that. lol that was so funny.
Awesome!!!!!!!!!!!!!!!
LOVELY
@wizard101Gamezhere1 7) 3:00 ''Eleven fairies dusting'' (Not ''fairys'') + On ''the'' 11th Day
8) 1:38 From there it says: On the seventh day of Christmas my true love gave to me seven sorts of jelly. And ONLY on the 12th day of Christmas it is "Seven dwarfs a jamming'' . 9) The TITLE of the song. It's CHRISTMAS (Not "Chirstmas") And there were several other tiny mistakes which I didn't mention.