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How Many Generic Chickens Can You Fit Into a Generic Pontiac?
A while back, someone asked how many generic chickens would fit
into a generic Pontiac. This question has been on my mind recently, so I
decided to work out this problem, for the benefit of all humanity.
I. It has been proven succesfully that chickens have a definite
wave-like nature. In reproducing Thomas Young's famous double-slit
experiment of 1801, Sir Kenneth Harbour-Thomas showed that chickens
not only diffract, but produce interference patterns as well. (This
experiment is fully documented in Sir Kenneth's famous treatise
"Tossing Chickens Through Various Apertures in Modern Architecture",
1897)
II. It is also known, as any farmhand can tell you, that whereas if one
chicken is placed in an enclosed space, it will be impossible to
pinpoint the exact location of the chicken at any given time t. This
was summarized by Helmut Heisenberg (Werner's younger brother) in
the equation:
d(chicken) * dt >= b
(where b is the barnyard constant; 5.2 x10^(-14) domestic fowl *
seconds)
III. Whatever our results, they must be consistant with the fundamentals
of physics, so energy, momentum, and charge must all be conserved.
A. Chickens (fortunately) do not carry electric charge. This was
discovered by Benjamin Franklin, after repeated experiments with
chickens, kites, and thunderstorms.
B. The total energy of a chicken is given by the equation:
E = K + V
Where V is the potential energy of the chicken, and K is the
kinetic energy of the chicken, given by
(.5)mv^2 or (p^2) / (2m).
C. Since chickens have an associated wavelength, w, we know that
the momentum of a free-chicken (that is, a chicken not enclosed
in any sort of Pontiac) is given by: p = b / w.
IV. With this in mind, it is possible to come up with a wave equation
for the potential energy of a generic chicken. (A wave equation will
allow us to calculate the probability of finding any number of
chickens in automobiles.) The wave equation for a non-relativistic,
time-independant chicken in a one- dimensional Pontiac is given by:
[V * P] - [[(b^2) / (2m)] * D^2(P)] = E * P
P is the wave function, and D^2(P) is its second derivative.
The wave equation can be used to prove that chickens are in
fact quantized, and that by using the Perdue Exclusion formula
we know that no two chickens in any Pontiac can have the same
set of quantum numbers.
V. The probability of finding a chicken in the Pontiac is simply the
integral of P * P * dChicken from 0 to x, where x = the length of the
Pontiac. Since each chicken will have its own set of quantum numbers
(when examining the case of the three-dimensional Pontiac) different
wave functions can be derived for each set of quantum numbers.
It is important to note that we now know that there is no such
thing as a generic chicken. Each chicken influences the position and
velocity of every other chicken inside the Pontiac, and each chicken
must be treated individually.
It has been theorized that chickens do in fact have an intrinsic
angular momentum, yet no experiment has been yet conducted to prove
this, as chickens tend to move away from someone trying to spin them.
Curious sidenote: Whenever possible, any attempt to integrate a
chicken should be done by parts, as most people will tend to want the
legs (dark meat), which can lead to innumerable family conflicts
which are best avoided if at all possible.
The Prestidigitator, Drew Physics Major Extraordinary
24 March 1988