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	<title>TTAN TTAKUN IRRATIA 107.2 FM &#187; The Confidential Frequencies</title>
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	<itunes:author>TTAN TTAKUN IRRATIA 107.2 FM</itunes:author>
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		<title>TTAN TTAKUN IRRATIA 107.2 FM &#187; The Confidential Frequencies</title>
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		<title>THECONFIDENTIALFREQUENCIES20130517</title>
		<link>http://ttanttakun.com/2013/05/theconfidentialfrequencies20130517-2</link>
		<comments>http://ttanttakun.com/2013/05/theconfidentialfrequencies20130517-2#comments</comments>
		<pubDate>Mon, 20 May 2013 12:42:13 +0000</pubDate>
		<dc:creator>Andy</dc:creator>
				<category><![CDATA[Irratsaioak]]></category>
		<category><![CDATA[The Confidential Frequencies]]></category>
		<category><![CDATA[1]]></category>
		<category><![CDATA[2]]></category>
		<category><![CDATA[a + τ]]]></category>
		<category><![CDATA[a + τ] The following formula]]></category>
		<category><![CDATA[a + τ]. It follows that if h(x) is τ-periodic]]></category>
		<category><![CDATA[a1] for x1]]></category>
		<category><![CDATA[a2]]></category>
		<category><![CDATA[a2 and a3. In particular]]></category>
		<category><![CDATA[a2 lies in the x-y plane]]></category>
		<category><![CDATA[a3 respectively: g(x_1]]></category>
		<category><![CDATA[and a = −τ/2. Another commonly used frequency domain representation uses the Fourier series coefficients to modulate a Dirac comb: G(f) \ \stackrel{\mathrm{def}}{=} \ \sum_{n=-\infty}^\infty G[n]\cdot]]></category>
		<category><![CDATA[and a is an arbitrary choice. Two popular choices are a = 0]]></category>
		<category><![CDATA[and a3 has components of all three axes). The denominator is exactly the volume of the primitive unit cell which is enclosed by the three primitive-vectors a1]]></category>
		<category><![CDATA[and functional notation often replaces subscripting: \begin{align} f(x) &= \sum_{n=-\infty}^\infty \hat{f}(n)\cdot e^{inx} \\ &= \sum_{n=-\infty}^\infty F[n]\cdot e^{jnx} &&\scriptstyl]]></category>
		<category><![CDATA[and z in terms of x1]]></category>
		<category><![CDATA[as follows: G[n] = \frac{1}{\tau}\int_a^{a+\tau} h(x)\cdot e^{-i 2\pi \frac{n}{\tau} x}\]]></category>
		<category><![CDATA[bn]]></category>
		<category><![CDATA[b_n = i( c_{n} - c_{-n} ) \quad \text{ for }n=1]]></category>
		<category><![CDATA[cn are related via a_n = { c_n + c_{-n} } \quad \text{ for }n=0]]></category>
		<category><![CDATA[c_n = \begin{cases} \frac{1}{2}(a_n - i b_n) & n > 0 \\ \quad \frac{1}{2}a_0 & n = 0 \\ \frac{1}{2}(a_{-n} + i b_{-n}) & n < 0. \end{cases} The notation cn is inadequate for discussi]]></category>
		<category><![CDATA[c_{j]]></category>
		<category><![CDATA[df]]></category>
		<category><![CDATA[dx]]></category>
		<category><![CDATA[dx. The basic Fourier series result for Hilbert spaces can be written as f=\sum_{n=-\infty}^\infty \langle f]]></category>
		<category><![CDATA[dx. The Fourier coefficients an]]></category>
		<category><![CDATA[dx_1 And then we could write: g(x_1]]></category>
		<category><![CDATA[dx_2 = \frac{1}{a_2}\int_0^{a_2} dx_2 \frac{1}{a_1}\int_0^{a_1} dx_1 g(x_1]]></category>
		<category><![CDATA[dx_3 = \frac{1}{a_3}\int_0^{a_3} dx_3 \frac{1}{a_2}\int_0^{a_2} dx_2 \frac{1}{a_1}\int_0^{a_1} dx_1 g(x_1]]></category>
		<category><![CDATA[dy. Aside from being useful for solving partial differential equations such as the heat equation]]></category>
		<category><![CDATA[each of which has periodicity a1]]></category>
		<category><![CDATA[even though the Fourier integral of a periodic function is not convergent at the harmonic frequencies.[nb 3] Fourier series on a square We can also define the Fourier series for functions of two varia]]></category>
		<category><![CDATA[every reciprocal lattice vector can be written as \mathbf{K} = l_{1}\mathbf{g}_{1} + l_{2}\mathbf{g}_{2} + l_{3}\mathbf{g}_{3}]]></category>
		<category><![CDATA[except possibly at discontinuities]]></category>
		<category><![CDATA[e^{inx} = \cos(nx)+i\sin(nx)]]></category>
		<category><![CDATA[e_n \rangle \]]></category>
		<category><![CDATA[e_n.]]></category>
		<category><![CDATA[f has units of hertz. The "teeth" of the comb are spaced at multiples (i.e. harmonics) of 1/τ]]></category>
		<category><![CDATA[f(r)]]></category>
		<category><![CDATA[for any positive integer n. Exponential Fourier series We can use Euler's formula]]></category>
		<category><![CDATA[for example]]></category>
		<category><![CDATA[g \rangle \;\stackrel{\mathrm{def}}{=} \; \frac{1}{2\pi}\int_{-\pi}^{\pi} f(x)\overline{g(x)}\]]></category>
		<category><![CDATA[g(x_1]]></category>
		<category><![CDATA[h(x)]]></category>
		<category><![CDATA[in which it just so happens that a1 is parallel to the x axis]]></category>
		<category><![CDATA[instead of with the x1]]></category>
		<category><![CDATA[is a periodic function with period τ on all of R: g(x)=\sum_{n=-\infty}^\infty G[n]\cdot e^{i 2\pi \frac{n}{\tau} x}. If a function is square-integrable in the interval [a]]></category>
		<category><![CDATA[is now a function of three-variables]]></category>
		<category><![CDATA[it can be represented in that interval by the formula above. I.e.]]></category>
		<category><![CDATA[k \in \mathbf{Z}\text{ (integers)}} c_{j]]></category>
		<category><![CDATA[k} = {1 \over 4 \pi^2} \int_{-\pi}^\pi \int_{-\pi}^\pi f(x]]></category>
		<category><![CDATA[k}e^{ijx}e^{iky}]]></category>
		<category><![CDATA[m_2]]></category>
		<category><![CDATA[m_3 \in \mathbf{Z} } h^{three}(m_1]]></category>
		<category><![CDATA[m_3) := \frac{1}{a_3}\int_0^{a_3} h^{two}(m_1]]></category>
		<category><![CDATA[m_3) \cdot e^{i 2\pi ( \frac{m_1}{a_1} x_1+ \frac{m_2}{a_2} x_2 + \frac{m_3}{a_3} x_3)}. Now]]></category>
		<category><![CDATA[m_3) \cdot e^{i 2\pi \frac{m_1}{a_1} x_1} \cdot e^{i 2\pi \frac{m_2}{a_2} x_2}\cdot e^{i 2\pi \frac{m_3}{a_3} x_3} Re-arranging: g(x_1]]></category>
		<category><![CDATA[one notable application of Fourier series on the square is in image compression. In particular]]></category>
		<category><![CDATA[particularly when the variable x represents time]]></category>
		<category><![CDATA[sinh is the hyperbolic sine function. This solution of the heat equation is obtained by multiplying each term of Eq.1 by sinh(ny)/sinh(nπ). While our example function f(x) seems to have a needlessly c]]></category>
		<category><![CDATA[such as \scriptstyle\hat{f} or F]]></category>
		<category><![CDATA[such that it obeys the following condition for any Bravais lattice vector R: f(r) = f(r+R)]]></category>
		<category><![CDATA[T(x]]></category>
		<category><![CDATA[the coefficient sequence is called a frequency domain representation. Square brackets are often used to emphasize that the domain of this function is a discrete set of frequencies. Fourier series on a]]></category>
		<category><![CDATA[the effective potential that one electron "feels" inside a periodic crystal. It is useful to make a Fourier series of the potential then when applying Bloch's theorem. First]]></category>
		<category><![CDATA[the Fourier coefficients are then given by: c_n = \frac{1}{2\pi}\int_{-\pi}^{\pi} f(x) e^{-inx}\]]></category>
		<category><![CDATA[the heat distribution T(x]]></category>
		<category><![CDATA[the jpeg image compression standard uses the two-dimensional discrete cosine transform]]></category>
		<category><![CDATA[the set of functions {en = einx; n ∈ Z} is an orthonormal basis for the space L2([−π]]></category>
		<category><![CDATA[the sum is actually over reciprocal lattice vectors: f(\mathbf{r})=\sum_{\mathbf{K}} h(\mathbf{K}) \cdot e^{i \mathbf{K} \cdot \mathbf{r}}. Where h(\mathbf{K}) = \frac{1}{a_3}\int_0^{a_3} dx_3 \frac{1]]></category>
		<category><![CDATA[their scalar product is: \mathbf{K} \cdot \mathbf{r} = \left ( l_{1}\mathbf{g}_{1} + l_{2}\mathbf{g}_{2} + l_{3}\mathbf{g}_{3} \right ) \cdot \left (x_1\frac{\mathbf{a}_{1}}{a_1}+ x_2\frac{\mathbf{a}_]]></category>
		<category><![CDATA[then g(x) will equal h(x) in the interval [a]]></category>
		<category><![CDATA[then: g(x) and h(x) are equal everywhere]]></category>
		<category><![CDATA[thus]]></category>
		<category><![CDATA[to give a more concise formula: f(x) = \sum_{n=-\infty}^ \infty c_n e^{inx}. Assuming f(x) is a periodic function with T = 2π]]></category>
		<category><![CDATA[to work in such a cartesian coordinate system]]></category>
		<category><![CDATA[we can calculate Jacobian determinant: \begin{bmatrix} \dfrac{\partial x_1}{\partial x} & \dfrac{\partial x_1}{\partial y} & \dfrac{\partial x_1}{\partial z} \\[3pt] \dfrac{\partial x_2}{\part]]></category>
		<category><![CDATA[we can define the following: h^{one}(m_1]]></category>
		<category><![CDATA[we can solve this system of three linear equations for x]]></category>
		<category><![CDATA[we can use the fact that \mathbf{g_i} \cdot \mathbf{a_j}=2\pi\delta_{ij} to calculate that for any arbitrary reciprocal lattice vector K and arbitrary vector in space r]]></category>
		<category><![CDATA[we could make a Fourier series of it. This kind of function can be]]></category>
		<category><![CDATA[we define: h^{three}(m_1]]></category>
		<category><![CDATA[we may write any arbitrary vector r in the coordinate-system of the lattice: \mathbf{r} = x_1\frac{\mathbf{a}_{1}}{a_1}+ x_2\frac{\mathbf{a}_{2}}{a_2}+ x_3\frac{\mathbf{a}_{3}}{a_3}]]></category>
		<category><![CDATA[we now know that dx_1 dx_2 dx_3 = \frac{a_1 a_2 a_3}{\mathbf{a_1}\cdot(\mathbf{a_2} \times \mathbf{a_3})} \cdot dx dy dz. We can write now h(K) as an integral with the traditional coordinate system ov]]></category>
		<category><![CDATA[when the coefficients are derived from a function]]></category>
		<category><![CDATA[where ai = |ai|. Thus we can define a new function]]></category>
		<category><![CDATA[where i is the imaginary unit]]></category>
		<category><![CDATA[where li are integers and gi are the reciprocal lattice vectors]]></category>
		<category><![CDATA[where variable f represents a continuous frequency domain. When variable x has units of seconds]]></category>
		<category><![CDATA[which is a Fourier transform using the cosine basis functions. Fourier series of Bravais-lattice-periodic-function The Bravais lattice is defined as the set of vectors of the form: \mathbf{R} = n_{1}\]]></category>
		<category><![CDATA[which is called the fundamental frequency. g(x) can be recovered from this representation by an inverse Fourier transform: \begin{align} \mathcal{F}^{-1}\{G(f)\} &= \int_{-\infty}^\infty \left( \s]]></category>
		<category><![CDATA[with appropriate complex-valued coefficients G[n]]]></category>
		<category><![CDATA[x2 and x3]]></category>
		<category><![CDATA[x2 and x3 in order to calculate the volume element in the original cartesian coordinate system. Once we have x]]></category>
		<category><![CDATA[x2 and x3 variables: h(\mathbf{K}) = \frac{1}{\mathbf{a_1}\cdot(\mathbf{a_2} \times \mathbf{a_3})}\int_{C} d\mathbf{r} f(\mathbf{r})\cdot e^{-i \mathbf{K} \cdot \mathbf{r}} And C is the primitive unit]]></category>
		<category><![CDATA[x_2]]></category>
		<category><![CDATA[x_2+a_2]]></category>
		<category><![CDATA[x_3)]]></category>
		<category><![CDATA[x_3) := f(\mathbf{r}) = f \left (x_1\frac{\mathbf{a}_{1}}{a_1}+x_2\frac{\mathbf{a}_{2}}{a_2}+x_3\frac{\mathbf{a}_{3}}{a_3} \right ). This new function]]></category>
		<category><![CDATA[x_3) := \frac{1}{a_1}\int_0^{a_1} g(x_1]]></category>
		<category><![CDATA[x_3) := \frac{1}{a_2}\int_0^{a_2} h^{one}(m_1]]></category>
		<category><![CDATA[x_3) = g(x_1]]></category>
		<category><![CDATA[x_3) = g(x_1+a_1]]></category>
		<category><![CDATA[x_3) \cdot e^{i 2\pi \frac{m_1}{a_1} x_1} Further defining: h^{two}(m_1]]></category>
		<category><![CDATA[x_3) \cdot e^{i 2\pi \frac{m_1}{a_1} x_1} \cdot e^{i 2\pi \frac{m_2} {a_2} x_2} And finally applying the same for the third coordinate]]></category>
		<category><![CDATA[x_3)=\sum_{m_1]]></category>
		<category><![CDATA[x_3)=\sum_{m_1=-\infty}^\infty h^{one}(m_1]]></category>
		<category><![CDATA[x_3)=\sum_{m_1=-\infty}^\infty \sum_{m_2=-\infty}^\infty h^{two}(m_1]]></category>
		<category><![CDATA[x_3)=\sum_{m_1=-\infty}^\infty \sum_{m_2=-\infty}^\infty \sum_{m_3=-\infty}^\infty h^{three}(m_1]]></category>
		<category><![CDATA[x_3)\cdot e^{-i 2\pi (\frac{m_1}{a_1} x_1+\frac{m_2}{a_2} x_2 + \frac{m_3}{a_3} x_3)} And write g as: g(x_1]]></category>
		<category><![CDATA[x_3)\cdot e^{-i 2\pi (\frac{m_1}{a_1} x_1+\frac{m_2}{a_2} x_2)} We can write g once again as: g(x_1]]></category>
		<category><![CDATA[x_3)\cdot e^{-i 2\pi \frac{m_1}{a_1} x_1}\]]></category>
		<category><![CDATA[x_3)\cdot e^{-i 2\pi \frac{m_2}{a_2} x_2}\]]></category>
		<category><![CDATA[x_3)\cdot e^{-i 2\pi \frac{m_3}{a_3} x_3}\]]></category>
		<category><![CDATA[x_3+a_3). If we write a series for g on the interval [0]]></category>
		<category><![CDATA[Y]]></category>
		<category><![CDATA[y) = 2\sum_{n=1}^\infty \frac{(-1)^{n+1}}{n} \sin(nx) {\sinh(ny) \over \sinh(n\pi)}. Here]]></category>
		<category><![CDATA[y) = \sum_{j]]></category>
		<category><![CDATA[y) e^{-ijx}e^{-iky}\]]></category>
		<category><![CDATA[y) is nontrivial. The function T cannot be written as a closed-form expression. This method of solving the heat problem was made possible by Fourier's work. Other applications Another application of t]]></category>
		<category><![CDATA[z) = x_1\frac{\mathbf{a}_{1}}{a_1}+x_2\frac{\mathbf{a}_{2}}{a_2}+x_3\frac{\mathbf{a}_{3}}{a_3}]]></category>
		<category><![CDATA[\]]></category>
		<category><![CDATA[\dots\]]></category>
		<category><![CDATA[\mathbf{a_1}\cdot(\mathbf{a_2} \times \mathbf{a_3}) is the volume of the primitive unit cell. Hilbert space interpretation Main article: Hilbert space In the language of Hilbert spaces]]></category>
		<category><![CDATA[\\ &= \sum_{n=-\infty}^\infty G[n]\cdot e^{i2\pi \frac{n}{\tau} x} \ \ \stackrel{\mathrm{def}}{=} \ g(x). \end{align} The function G(f) is therefore commonly referred to as a Fourier transform]]></category>
		<category><![CDATA[\\ &= \sum_{n=-\infty}^\infty G[n]\cdot \int_{-\infty}^\infty \delta\left(f-\frac{n}{\tau}\right) e^{i 2 \pi f x}\]]></category>
		<category><![CDATA[π]) of square-integrable functions of [−π]]></category>
		<category><![CDATA[π]. This space is actually a Hilbert space with an inner product given for any two elements f and g by: \langle f]]></category>
		<category><![CDATA[π]: f(x]]></category>
		<category><![CDATA[π]×[−π]]></category>

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<enclosure url="http://ia601708.us.archive.org/17/items/THECONFIDENTIALFREQUENCIES20130517/THECONFIDENTIALFREQUENCIES20130517.mp3" length="145054813" type="audio/mpeg" />
			<itunes:keywords>1,2,a + τ],a + τ] The following formula,a + τ]. It follows that if h(x) is τ-periodic,a1] for x1,a2,a2 and a3. In particular,a2 lies in the x-y plane,a3 respectively: g(x_1,and a = −τ/2. Another commonly used frequency domain representation uses the Fo...</itunes:keywords>
	<itunes:subtitle></itunes:subtitle>
		<itunes:summary></itunes:summary>
		<itunes:author>TTAN TTAKUN IRRATIA 107.2 FM</itunes:author>
		<itunes:explicit>no</itunes:explicit>
		<itunes:duration>1:00:26</itunes:duration>
	</item>
		<item>
		<title>THECONFIDENTIALFREQUENCIES20130301</title>
		<link>http://ttanttakun.com/2013/03/theconfidentialfrequencies20130301</link>
		<comments>http://ttanttakun.com/2013/03/theconfidentialfrequencies20130301#comments</comments>
		<pubDate>Sat, 09 Mar 2013 21:47:55 +0000</pubDate>
		<dc:creator>Andy</dc:creator>
				<category><![CDATA[Irratsaioak]]></category>
		<category><![CDATA[The Confidential Frequencies]]></category>
		<category><![CDATA[-20]]></category>
		<category><![CDATA[-35db levels.) Used as a delay/echo]]></category>
		<category><![CDATA[a single analog backlit VU meter for all three inputs]]></category>
		<category><![CDATA[A tape echo device records incoming audio to a loop of magnetic tape]]></category>
		<category><![CDATA[and intensity (number of repeats]]></category>
		<category><![CDATA[and still used by many bands to this day]]></category>
		<category><![CDATA[and the rockabilly stylings of Brian Setzer]]></category>
		<category><![CDATA[as well as dry and effected "Echo" output jacks with a switch for output setting (-10]]></category>
		<category><![CDATA[but made as one]]></category>
		<category><![CDATA[constantly moving jumble in the tape chamber (also known as the tape tank) under a plastic panel which protects the tape and keeps it from getting tangled. The replacement tapes were known as Roland R]]></category>
		<category><![CDATA[continuous loop. In the Roland 'RE' range there are no reels of any kind]]></category>
		<category><![CDATA[even without an input signal (by turning the intensity control to maximum and allowing the unit to self-regenerate]]></category>
		<category><![CDATA[in a sense; it actually reduces how much the erase/record head erases the tape)]]></category>
		<category><![CDATA[notably in the experimental work of Radiohead]]></category>
		<category><![CDATA[one instrument and two microphone inputs]]></category>
		<category><![CDATA[or self-oscillate]]></category>
		<category><![CDATA[repeat pattern (an 11-position rotary switch)]]></category>
		<category><![CDATA[that can be adjusted to a user's liking; and bass/treble controls to EQ the sound of the repeats (not the dry signal)]]></category>
		<category><![CDATA[the latter using one recently to get the slapback sound sought after for rockabilly and such styles of music. The Roland RE-201 is also extensively used in modern electronic music.[2]]]></category>
		<category><![CDATA[the Roland RE-201 is said to produce an unpredictable delay that is warm and gritty sounding. It is also capable of producing a large variety of its own sound effects]]></category>
		<category><![CDATA[the Roland RE-201 is widely sought after]]></category>
		<category><![CDATA[the tape is transported via a capstan drive. The tape loop is contained in a loose]]></category>
		<category><![CDATA[then replays the audio over a series of several playback heads before it is erased again by new incoming audio. The tape used in the RE-201 is the standard 1/4" tape of the open-reel variety]]></category>
		<category><![CDATA[wet/dry mix for both echo and reverb]]></category>
		<category><![CDATA[while manipulating the tape speed and other controls). Despite its age]]></category>

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			<itunes:keywords>-20,-35db levels.) Used as a delay/echo,a single analog backlit VU meter for all three inputs,A tape echo device records incoming audio to a loop of magnetic tape,and intensity (number of repeats,and still used by many bands to this day,</itunes:keywords>
	<itunes:subtitle></itunes:subtitle>
		<itunes:summary></itunes:summary>
		<itunes:author>TTAN TTAKUN IRRATIA 107.2 FM</itunes:author>
		<itunes:explicit>no</itunes:explicit>
		<itunes:duration>1:07:43</itunes:duration>
	</item>
		<item>
		<title>THECONFIDENTIALCOSMICMOONRADIOAMOR20130215</title>
		<link>http://ttanttakun.com/2013/02/theconfidentialcosmicmoonradioamor20130215</link>
		<comments>http://ttanttakun.com/2013/02/theconfidentialcosmicmoonradioamor20130215#comments</comments>
		<pubDate>Mon, 18 Feb 2013 20:01:08 +0000</pubDate>
		<dc:creator>Andy</dc:creator>
				<category><![CDATA[Irratsaioak]]></category>
		<category><![CDATA[The Confidential Frequencies]]></category>

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		<itunes:subtitle></itunes:subtitle>
		<itunes:summary></itunes:summary>
		<itunes:author>TTAN TTAKUN IRRATIA 107.2 FM</itunes:author>
		<itunes:explicit>no</itunes:explicit>
		<itunes:duration>1:12:40</itunes:duration>
	</item>
		<item>
		<title>THECONFIDENTIALFREQUENCIES20130208</title>
		<link>http://ttanttakun.com/2013/02/theconfidentialfrequencies20130208</link>
		<comments>http://ttanttakun.com/2013/02/theconfidentialfrequencies20130208#comments</comments>
		<pubDate>Sun, 10 Feb 2013 16:11:37 +0000</pubDate>
		<dc:creator>Andy</dc:creator>
				<category><![CDATA[Irratsaioak]]></category>
		<category><![CDATA[The Confidential Frequencies]]></category>
		<category><![CDATA[" which Boucher intended to be pronounced "sexy"]]></category>
		<category><![CDATA[Adaptec and Optimem were early supporters of the SCSI standard.[5] The NCR facility in Wichita]]></category>
		<category><![CDATA[and added it to its high-end desktops starting with the Power Macintosh G3 in 1997. Apple dropped on-board SCSI completely (in favor of IDE and FireWire) with the (Blue & White) Power Mac G3 in 19]]></category>
		<category><![CDATA[ANSI developed the specification as "SASI" and "Shugart Associates System Interface;"[5] however]]></category>
		<category><![CDATA[Apple Macintosh and Sun Microsystems computer lines and PC server systems. Apple started using Parallel ATA (also known as IDE) for its low-end machines with the Macintosh Quadra 630 in 1994]]></category>
		<category><![CDATA[but ENDL's[6] Dal Allan pronounced the new acronym as "scuzzy" and that stuck.[4] A number of companies such as NCR Corporation]]></category>
		<category><![CDATA[defined the interface as using a 50-pin flat ribbon connector which was adopted as the SCSI-1 connector. SASI is a fully compliant subset of SCSI-1 so that many]]></category>
		<category><![CDATA[developed c. 1978 and publicly disclosed in 1981.[2] A SASI controller provided a bridge between a hard disk drive's low-level interface and a host computer]]></category>
		<category><![CDATA[if not all]]></category>
		<category><![CDATA[Kansas is widely thought to have developed the industry's first SCSI chip; it worked the first time.[7] The "small" part in SCSI is historical; since the mid-1990s]]></category>
		<category><![CDATA[of the then-existing SASI controllers were SCSI-1 compatible.[3] Larry Boucher is considered to be the "father" of SASI and SCSI due to his pioneering work first at Shugart Associates and then at Adap]]></category>
		<category><![CDATA[owing to the lower cost and adequate performance of ATA hard disk standard. However]]></category>
		<category><![CDATA[SCSI drives and even SCSI RAIDs became common in PC workstations for video or audio production.]]></category>
		<category><![CDATA[SCSI has been available on even the largest of computer systems. Since its standardization in 1986]]></category>
		<category><![CDATA[SCSI has been commonly used in the Amiga]]></category>
		<category><![CDATA[SCSI was derived from "SASI"]]></category>
		<category><![CDATA[the "Shugart Associates System Interface"]]></category>
		<category><![CDATA[the committee documenting the standard would not allow it to be named after a company. Almost a full day was devoted to agreeing to name the standard "Small Computer System Interface]]></category>
		<category><![CDATA[which needed to read blocks of data. SASI controller boards were typically the size of a hard disk drive and were usually physically mounted to the drive's chassis. SASI]]></category>
		<category><![CDATA[which was used in mini- and early microcomputers]]></category>

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			<itunes:keywords>&quot; which Boucher intended to be pronounced &quot;sexy&quot;,Adaptec and Optimem were early supporters of the SCSI standard.[5] The NCR facility in Wichita,and added it to its high-end desktops starting with the Power Macintosh G3 in 1997.</itunes:keywords>
	<itunes:subtitle></itunes:subtitle>
		<itunes:summary></itunes:summary>
		<itunes:author>TTAN TTAKUN IRRATIA 107.2 FM</itunes:author>
		<itunes:explicit>no</itunes:explicit>
		<itunes:duration>1:07:39</itunes:duration>
	</item>
		<item>
		<title>THECONFIDENTIALFREQUENCIES20130125</title>
		<link>http://ttanttakun.com/2013/01/theconfidentialfrequencies20130125</link>
		<comments>http://ttanttakun.com/2013/01/theconfidentialfrequencies20130125#comments</comments>
		<pubDate>Sun, 27 Jan 2013 10:56:35 +0000</pubDate>
		<dc:creator>Andy</dc:creator>
				<category><![CDATA[Irratsaioak]]></category>
		<category><![CDATA[The Confidential Frequencies]]></category>
		<category><![CDATA[a glitch is a programming error which results in behavior not intended by the programmers. (An example of this is getting to fight MissingNo. from Pokémon Red and Blue; not only is the existence of Mi]]></category>
		<category><![CDATA[and other issues. Graphical glitches are especially notorious in platforming games]]></category>
		<category><![CDATA[and then compiling reports on the glitches to be fed back to the programmers so that they can repair the bugs.[6]]]></category>
		<category><![CDATA[but encountering MissingNo. causes graphical and inventory glitches.) Glitches may include incorrectly displayed graphics]]></category>
		<category><![CDATA[by displaying a harmless ground texture where the code calls for an area that should damage the character]]></category>
		<category><![CDATA[carries the risk of crashing the game or even causing permanent damage to the game medium.[8] Part of the quality assurance process (as performed by game testers for video games) is locating and repro]]></category>
		<category><![CDATA[collision detection errors]]></category>
		<category><![CDATA[game freezes/crashes]]></category>
		<category><![CDATA[however]]></category>
		<category><![CDATA[In video games]]></category>
		<category><![CDATA[music]]></category>
		<category><![CDATA[or by not displaying a wall texture where there should be one]]></category>
		<category><![CDATA[or gameplay glitches. Doing this]]></category>
		<category><![CDATA[resulting in an invisible wall).Some glitches are potentially dangerous to the game save data.[6] "Glitching" is the practice of a player exploiting faults in a video game's programming to achieve tas]]></category>
		<category><![CDATA[sound issues]]></category>
		<category><![CDATA[such as running through walls or defying the game's laws of gravity. It is often used to gain an unfair advantage over other players in multiplayer video games. Glitches can be deliberately induced in]]></category>
		<category><![CDATA[such as tilting a ROM cartridge to disconnect one or more connections along the edge connector and interrupt part of the flow of data between the cartridge and the console.[7] This can result in graph]]></category>
		<category><![CDATA[where misformed textures can directly affect gameplay (for example]]></category>

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		<description><![CDATA[]]></description>
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			<itunes:keywords>a glitch is a programming error which results in behavior not intended by the programmers. (An example of this is getting to fight MissingNo. from Pokémon Red and Blue; not only is the existence of Mi,and other issues.</itunes:keywords>
	<itunes:subtitle></itunes:subtitle>
		<itunes:summary></itunes:summary>
		<itunes:author>TTAN TTAKUN IRRATIA 107.2 FM</itunes:author>
		<itunes:explicit>no</itunes:explicit>
		<itunes:duration>1:16:18</itunes:duration>
	</item>
		<item>
		<title>THECONFIDENTIALFREQUENCIES20130104</title>
		<link>http://ttanttakun.com/2013/01/theconfidentialfrequencies20130104</link>
		<comments>http://ttanttakun.com/2013/01/theconfidentialfrequencies20130104#comments</comments>
		<pubDate>Fri, 04 Jan 2013 20:25:23 +0000</pubDate>
		<dc:creator>Andy</dc:creator>
				<category><![CDATA[Irratsaioak]]></category>
		<category><![CDATA[The Confidential Frequencies]]></category>
		<category><![CDATA[35MHz]]></category>
		<category><![CDATA[49MHz]]></category>
		<category><![CDATA[and 72MHz. Spektrum systems are distinguished in that they use Spread Spectrum technology on the 2.4GHz ISM band. Spektrum refers to their technology as "Digital Spectrum Modulation." Each transmitter]]></category>
		<category><![CDATA[and Europe typically employs FM radio control in HF and VHF bands such as 27MHz]]></category>
		<category><![CDATA[ensuring that no transmitter will interfere with other nearby Spektrum DSMx systems. This works in a manner that both transmitter and receiver are constantly changing through the different frequencies]]></category>
		<category><![CDATA[japan]]></category>
		<category><![CDATA[Spektrum is brand of radio control systems designed for use with hobby radio-controlled cars and aircraft. Spektrum is a division of Horizon Hobby. The R/C hobby in the United States]]></category>
		<category><![CDATA[to which receivers can be bound]]></category>

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			<itunes:keywords>35MHz,49MHz,and 72MHz. Spektrum systems are distinguished in that they use Spread Spectrum technology on the 2.4GHz ISM band. Spektrum refers to their technology as &quot;Digital Spectrum Modulation.&quot; Each transmitter,</itunes:keywords>
	<itunes:subtitle></itunes:subtitle>
		<itunes:summary></itunes:summary>
		<itunes:author>TTAN TTAKUN IRRATIA 107.2 FM</itunes:author>
		<itunes:explicit>no</itunes:explicit>
		<itunes:duration>1:00:01</itunes:duration>
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		<title>THECONFIDENTIALFREQUENCIES20121214_opiumradiophonicstations</title>
		<link>http://ttanttakun.com/2012/12/theconfidentialfrequencies20121214_opiumradiophonicstations</link>
		<comments>http://ttanttakun.com/2012/12/theconfidentialfrequencies20121214_opiumradiophonicstations#comments</comments>
		<pubDate>Tue, 18 Dec 2012 00:49:25 +0000</pubDate>
		<dc:creator>Andy</dc:creator>
				<category><![CDATA[Irratsaioak]]></category>
		<category><![CDATA[The Confidential Frequencies]]></category>
		<category><![CDATA[a proposed propulsion system for interplanetary travel. Planets are too massive for their trajectories to be significantly affected by these forces]]></category>
		<category><![CDATA[although their atmospheres are eroded by the solar winds. All of the observable universe is filled with large numbers of photons]]></category>
		<category><![CDATA[and as such]]></category>
		<category><![CDATA[and is the closest physical approximation of a perfect vacuum. But no vacuum is truly perfect]]></category>
		<category><![CDATA[and quite likely a correspondingly large number of neutrinos. The current temperature of this radiation is about 3 K]]></category>
		<category><![CDATA[and varies greatly due to space weather. Astrophysicists prefer to use number density to describe these environments]]></category>
		<category><![CDATA[atmospheres have no clearly delineated boundary: the density of atmospheric gas simply decreases with distance from the object. The Earth's atmospheric pressure drops to about 3.2 × 10−2 Pa at 100 kil]]></category>
		<category><![CDATA[in units of particles per cubic centimetre. But although it meets the definition of outer space]]></category>
		<category><![CDATA[isotropic gas pressure rapidly becomes insignificant when compared to radiation pressure from the sun and the dynamic pressure of the solar wind]]></category>
		<category><![CDATA[not even in interstellar space]]></category>
		<category><![CDATA[or -270 degrees Celsius or -454 degrees Fahrenheit.]]></category>
		<category><![CDATA[Outer space has very low density and pressure]]></category>
		<category><![CDATA[planets and moons keep their atmospheres by gravitational attraction]]></category>
		<category><![CDATA[so the definition of pressure becomes difficult to interpret. The thermosphere in this range has large gradients of pressure]]></category>
		<category><![CDATA[temperature and composition]]></category>
		<category><![CDATA[the atmospheric density within the first few hundred kilometers above the Kármán line is still sufficient to produce significant drag on satellites. Most artificial satellites operate in this region c]]></category>
		<category><![CDATA[the so-called cosmic background radiation]]></category>
		<category><![CDATA[where there are still a few hydrogen atoms per cubic meter.[4] Stars]]></category>
		<category><![CDATA[which is a common definition of the boundary with outer space. Beyond this line]]></category>
		<category><![CDATA[[22] the Kármán line]]></category>

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			<itunes:keywords>a proposed propulsion system for interplanetary travel. Planets are too massive for their trajectories to be significantly affected by these forces,although their atmospheres are eroded by the solar winds. All of the observable universe is filled with ...</itunes:keywords>
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		<itunes:summary></itunes:summary>
		<itunes:author>TTAN TTAKUN IRRATIA 107.2 FM</itunes:author>
		<itunes:explicit>no</itunes:explicit>
		<itunes:duration>1:33:52</itunes:duration>
	</item>
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		<title>THECONFIDENTIALFREQUENCIES20121123</title>
		<link>http://ttanttakun.com/2012/11/theconfidentialfrequencies20121123</link>
		<comments>http://ttanttakun.com/2012/11/theconfidentialfrequencies20121123#comments</comments>
		<pubDate>Sat, 24 Nov 2012 15:17:58 +0000</pubDate>
		<dc:creator>Andy</dc:creator>
				<category><![CDATA[Irratsaioak]]></category>
		<category><![CDATA[The Confidential Frequencies]]></category>
		<category><![CDATA[although it largely fell out of favour in about the tenth century AD when two drawn round wires]]></category>
		<category><![CDATA[and so producing wire of incorrect diameter. Diamond dies must be rebored when they have lost their original diameter of hole]]></category>
		<category><![CDATA[appeared in the Eastern Mediterranean and Italy in the seventh century BC]]></category>
		<category><![CDATA[but metal dies are brought down to size again by hammering up the hole and then drifting it out to correct diameter with a punch.]]></category>
		<category><![CDATA[if not technically advanced]]></category>
		<category><![CDATA[In antiquity]]></category>
		<category><![CDATA[in the form of chains and applied decoration]]></category>
		<category><![CDATA[jewelry often contains]]></category>
		<category><![CDATA[large amounts of wire that is accurately made and which must have been produced by some efficient]]></category>
		<category><![CDATA[manufactured goods whose import was prohibited by Edward IV in 1463.[4] The first wire mill in Great Britain was established at Tintern in about 1568 by the founders of the Company of Mineral and Batt]]></category>
		<category><![CDATA[means. In some cases]]></category>
		<category><![CDATA[or between a grooved punch and a grooved metal anvil. Swaging is of great antiquity]]></category>
		<category><![CDATA[or for fine work it may be a diamond or a ruby. The object of utilising precious stones is to enable the dies to be used for a considerable period without losing their size]]></category>
		<category><![CDATA[perhaps disseminated by the Phoenicians. Beaded wire continued to be used in jewellery into modern times]]></category>
		<category><![CDATA[possibly dating to the beginning of the 2nd millennium BC in Egypt and in the Bronze and Iron Ages in Europe for torcs and fibulae. Twisted square section wires are a very common filigree decoration i]]></category>
		<category><![CDATA[produced by mechanically distorting a round-section wire]]></category>
		<category><![CDATA[provided a simpler-to-make alternative. A forerunner to beaded wire may be the notched strips and wires which first occur from around 2000 BC in Anatolia. Wire was drawn in England from the medieval p]]></category>
		<category><![CDATA[strips cut from metal sheet were made into wire by pulling them through perforations in stone beads. This causes the strips to fold round on themselves to form thin tubes. This strip drawing technique]]></category>
		<category><![CDATA[the drawing of wire down to fine sizes continued to be done manually. Wire is usually drawn of cylindrical form; but it may be made of any desired section by varying the outline of the holes in the dr]]></category>
		<category><![CDATA[twisted together to form what are termed 'ropes']]></category>
		<category><![CDATA[who had a monopoly on this.[5] Apart from their second wire mill at nearby Whitebrook]]></category>
		<category><![CDATA[[6] there were no other wire mills before the second half of the 17th century. Despite the existence of mills]]></category>

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			<itunes:keywords>although it largely fell out of favour in about the tenth century AD when two drawn round wires,and so producing wire of incorrect diameter. Diamond dies must be rebored when they have lost their original diameter of hole,</itunes:keywords>
	<itunes:subtitle></itunes:subtitle>
		<itunes:summary></itunes:summary>
		<itunes:author>TTAN TTAKUN IRRATIA 107.2 FM</itunes:author>
		<itunes:explicit>no</itunes:explicit>
		<itunes:duration>1:24:32</itunes:duration>
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		<title>THECONFIDENTIALFREQUENCIES20121116</title>
		<link>http://ttanttakun.com/2012/11/theconfidentialfrequencies20121116</link>
		<comments>http://ttanttakun.com/2012/11/theconfidentialfrequencies20121116#comments</comments>
		<pubDate>Fri, 16 Nov 2012 23:57:15 +0000</pubDate>
		<dc:creator>Andy</dc:creator>
				<category><![CDATA[Irratsaioak]]></category>
		<category><![CDATA[The Confidential Frequencies]]></category>
		<category><![CDATA["where life has no value".]]></category>
		<category><![CDATA[abstract law]]></category>
		<category><![CDATA[although some notable examples (e.g. the later Westerns of John Ford or Clint Eastwood's Unforgiven) are more morally ambiguous. Westerns often stress the harshness of the wilderness and frequently se]]></category>
		<category><![CDATA[as Sergio Leone said]]></category>
		<category><![CDATA[brawling and shooting. In some Westerns]]></category>
		<category><![CDATA[desolate landscape. Specific settings include isolated forts]]></category>
		<category><![CDATA[direct or private justice (such as the feud[2])]]></category>
		<category><![CDATA[drinking (beer or whiskey)]]></category>
		<category><![CDATA[fighting villains of various kinds and bound to no fixed social structures but only to his own innate code of honor. And like knights errant]]></category>
		<category><![CDATA[gambling (draw poker or five card stud)]]></category>
		<category><![CDATA[general store]]></category>
		<category><![CDATA[in which social order is maintained predominately through relatively impersonal institutions. The popular perception of the Western is a story that centers on the life of a semi-nomadic wanderer]]></category>
		<category><![CDATA[it is]]></category>
		<category><![CDATA[it is usually the saloon that emphasizes that this is the "Wild West": it is the place to go for music (raucous piano playing)]]></category>
		<category><![CDATA[livery stable and jailhouse. Apart from the wilderness]]></category>
		<category><![CDATA[ranches and homesteads; the Native American village; or the small frontier town with its saloon]]></category>
		<category><![CDATA[rather than one organized around rationalistic]]></category>
		<category><![CDATA[such protagonists may be considered the literary descendants of the knight errant which stood at the center of earlier extensive genres such as the Arthurian Romances.[1] Like the cowboy or gunfighter]]></category>
		<category><![CDATA[the heroes of Westerns frequently rescue damsels in distress. Similarly]]></category>
		<category><![CDATA[the knight errant of the earlier European tales and poetry was wandering from place to place on his horse]]></category>
		<category><![CDATA[the town has a church and a school; in others]]></category>
		<category><![CDATA[the wandering protagonists of Westerns share many of the characteristics equated with the image of the ronin in modern Japanese culture. The Western typically takes these elements and uses them to tel]]></category>
		<category><![CDATA[The Western genre sometimes portrays the conquest of the wilderness and the subordination of nature in the name of civilization or the confiscation of the territorial rights of the original inhabitant]]></category>
		<category><![CDATA[usually a cowboy or a gunfighter.[1] In some ways]]></category>
		<category><![CDATA[where "civilization" has arrived]]></category>
		<category><![CDATA[where frontier rules still hold sway]]></category>
		<category><![CDATA[women (often prostitutes)]]></category>

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			<itunes:keywords>&quot;where life has no value&quot;.,abstract law,although some notable examples (e.g. the later Westerns of John Ford or Clint Eastwood&#039;s Unforgiven) are more morally ambiguous. Westerns often stress the harshness of the wilderness and frequently se,</itunes:keywords>
	<itunes:subtitle></itunes:subtitle>
		<itunes:summary></itunes:summary>
		<itunes:author>TTAN TTAKUN IRRATIA 107.2 FM</itunes:author>
		<itunes:explicit>no</itunes:explicit>
		<itunes:duration>1:19:06</itunes:duration>
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		<title>THECONFIDENTIALFREQUENCIES20121109</title>
		<link>http://ttanttakun.com/2012/11/theconfidentialfrequencies20121109</link>
		<comments>http://ttanttakun.com/2012/11/theconfidentialfrequencies20121109#comments</comments>
		<pubDate>Sat, 10 Nov 2012 15:30:09 +0000</pubDate>
		<dc:creator>Andy</dc:creator>
				<category><![CDATA[Irratsaioak]]></category>
		<category><![CDATA[The Confidential Frequencies]]></category>
		<category><![CDATA["Étude aux chemins de fer"]]></category>
		<category><![CDATA["Weekend")]]></category>
		<category><![CDATA[a collage of words]]></category>
		<category><![CDATA[allowing him to trigger and mix together the various train sounds as needed.[4] Sound collage became more common with the widespread use of magnetic tape in the early 1950s. Recording engineers soon d]]></category>
		<category><![CDATA[an artist well known for his use of collage in pieces including Contra Mortem et Tempus and Symphony No. 3 (Rochberg).[5]]]></category>
		<category><![CDATA[and centonization differ from collage in that the various elements in them are made to fit smoothly together]]></category>
		<category><![CDATA[and even from different sources. It wasn't long before artists began to explore the new possibilities. William S. Burroughs]]></category>
		<category><![CDATA[and Iannis Xenakis were early artists who experimented with it.[citation needed] The most famous examples in popular music are to be found in the work of The Beatles: George Martin cut up and randomly]]></category>
		<category><![CDATA[and Ives actually predates the use of collage in painting by artists like Picasso and Braque]]></category>
		<category><![CDATA[and John Lennon included a long pastiche of sound effects and crowd noises on The Beatles titled "Revolution 9".[citation needed] The cultural awareness of dada sound collage was greatly increased in ]]></category>
		<category><![CDATA[and some critics have described certain passages in Mahler symphonies as collage]]></category>
		<category><![CDATA[as in a film montage sequence. Although the technique of collage is generally associated with painting]]></category>
		<category><![CDATA[Brion Gysin]]></category>
		<category><![CDATA[but the first fully developed collages occur in a few works by Charles Ives. Earlier traditional forms and procedures such as the quodlibet]]></category>
		<category><![CDATA[composed in 1906]]></category>
		<category><![CDATA[creates the feeling of a walk in the city by layering several distinct melodies and quotations on top of each other. The first documented instance of sound collage created by electronic means is the p]]></category>
		<category><![CDATA[either by layering them or by moving between them in quick succession]]></category>
		<category><![CDATA[however]]></category>
		<category><![CDATA[in 1948]]></category>
		<category><![CDATA[in his piece Central Park in the Dark]]></category>
		<category><![CDATA[John Cage]]></category>
		<category><![CDATA[Mahler]]></category>
		<category><![CDATA[medley]]></category>
		<category><![CDATA[meter]]></category>
		<category><![CDATA[Mozart]]></category>
		<category><![CDATA[music and sounds created by film-maker and media artist Walter Ruttmann in 1928.[3] Later]]></category>
		<category><![CDATA[on the other hand]]></category>
		<category><![CDATA[or other discrepancies are important in helping to preserve the individuality of the constituent elements and to convey the impression of a heterogeneous assemblage.[2] What made their technique true ]]></category>
		<category><![CDATA[Pierre Schaeffer used the techniques of sound collage to create the first piece of musique concrète]]></category>
		<category><![CDATA[potpourri]]></category>
		<category><![CDATA[some of which had lock grooves allowing them to play in a continuous loop. He then set up multiple turntables in his studio]]></category>
		<category><![CDATA[tempo]]></category>
		<category><![CDATA[texture]]></category>
		<category><![CDATA[The origin of sound collage can be traced back to the works of Biber's programmatic sonata Battalia (1673) and Mozart's Don Giovanni (1789)]]></category>
		<category><![CDATA[the use of collage in music by Biber]]></category>
		<category><![CDATA[timbre]]></category>
		<category><![CDATA[was the juxtaposition of quotations and unrelated melodies]]></category>
		<category><![CDATA[whereas in a collage clashes of key]]></category>
		<category><![CDATA[which was assembled from recordings of trains. Schaeffer created this piece by recording sounds of trains onto several vinyl records]]></category>
		<category><![CDATA[who are generally credited with creating the first collage paintings around 1912. Ives]]></category>

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<enclosure url="http://ia601201.us.archive.org/3/items/THECONFIDENTIALFREQUENCIES20121109/THECONFIDENTIALFREQUENCIES20121109.mp3" length="691019776" type="audio/mpeg" />
			<itunes:keywords>&quot;Étude aux chemins de fer&quot;,&quot;Weekend&quot;),a collage of words,allowing him to trigger and mix together the various train sounds as needed.[4] Sound collage became more common with the widespread use of magnetic tape in the early 1950s.</itunes:keywords>
	<itunes:subtitle></itunes:subtitle>
		<itunes:summary></itunes:summary>
		<itunes:author>TTAN TTAKUN IRRATIA 107.2 FM</itunes:author>
		<itunes:explicit>no</itunes:explicit>
		<itunes:duration>4:47:55</itunes:duration>
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