If the current enters at X, it will pass along at E and be ready to leave at Y, as soon as E touches one of the contact points.
"How Two Boys Made Their Own Electrical Apparatus" by Thomas M. (Thomas Matthew) St. John
They are, like the current coordinates, x, y, numerical.
"Encyclopaedia Britannica, 11th Edition, Volume 11, Slice 6" by Various
Surrounding this core is a coil Y, which is connected with a source E of rapidly varying currents.
"The inventions, researches and writings of Nikola Tesla" by Thomas Commerford Martin
It may be asked: If the wires are passing currents to work the writing apparatus, how can they simultaneously affect the lifting-bar, Y?
"The Romance of Modern Invention" by Archibald Williams
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A survey of current practices of physicians who treat adductor spasmodic dysphonia in the U.S. May 1, 2009 by Christopher Y Chang, MD, Peter Chabot, PhD, and Christopher M Walz, MD.
The company, currently based in Briarcliff Manor, N.Y.
According to "Youth Development Current Trends," gay, lesbian or bisexual students were more than five times more likely to have attempted suicide in the past y.
This month's Cy Press Poetry session includes readings from Matvei Yankelevich (NYC), Jennifer Scappettone (Chicago) and Cincinnati native/current Brooklyn, N.Y. Resident Brett Price.
The Zoom Q3 Handy Video Recorder stands out from today's current crop of compact, affordable video recorders like the Flip and Vado by providing a pair of built-in X/Y-configured condenser microphones that record high-quality audio in stereo.
Laundrylux continues to provide hands-on help to laundry owners with its end-of-year Open House at its corporate office in Inwood, N.Y. Current store owners can visit anytime between 11 am and 4 pm to speak with Factory experts.
After reviewing the various proposals, I favor the design by T Y Lin as the best replacement for the current span.
Joe Klein has the Time cover story this week—a smart if very Joe Klein-y take on the ideological posturing of the current GOP primary field.
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Sekimoto K. and Nakazawa H. (1998): in Current Topics in Physics, Y.M.
Mechanical oscillations at the cellular scale
Expanding the current (M + Y )−1 yields In = h(m2 )−n i and an = Z n = Y n in the standard expansion (30) and In = hM −n i and bn = Zn in the generalized case (33).
Generalized heat kernel coefficients
Since y ≥ 0, a simple argument shows this is a lower bound on λ∗ = minx∈P maxj fj (x).) Notation: During the course of the algorithm, let ¯x denote the current solution Px∈S x/|S | represented by S .
Randomized Rounding without Solving the Linear Program
The current localization theory Now I brieﬂy review the existing theory for localization.
Are waves all localized in two dimensional random media?
Let f : Y → X be a surjective morphism and let T be a closed positive (1, 1)-current on X .
On Zariski decomposition problem
The current guess is that it is the result of which needs to be improved (we thank Y.
Stability of the Absolutely Continuous Spectrum of Random Schroedinger Operators on Tree Graphs
The entries on and above the diagonal of ρ(s) (ρj,k (s), 1 ≤ j ≤ k ≤ n) will be referred to as the upper entries; they correspond to the current ranks for pro jY (Y ).
Rank Independence and Rearrangements of Random Variables
Benjamini and Wilson’s proof of transience in two dimensions will play a crucial role in the current paper so let’s describe it brieﬂy.
Excited random walk in two dimensions has linear speed
Replace the current coordinate of y with U .
Nonparametric Bayesian Classification
For each coordinate of y do: Set U 1 = the current coordinate of y .
Nonparametric Bayesian Classification
If Y is a complex submanifold of X of codimension p, we let [Y ] ∈ D ′p,p(X ) denote the current of integration over Y given by ([Y ], ϕ) = RY ϕ. (For a further description of currents on complex manifolds, see [GH, Ch. 3].) We now suppose that S is base point free ; i.e., the set {z ∈ M : s(z) = 0, ∀s ∈ S } is empty.
Number variance of random zeros on complex manifolds
Unlike in the Y p,q case here we do not have SU (2) symmetry and we therefore cannot use the related current as an insertion in order to construct the relevant H = 1 operator.
On the pp-wave limit and the BMN structure of new Sasaki-Einstein spaces
Exactly like in the Y p,q case we have δH = 2 for these currents, since they are invariant under the U (1) isometries of the theory, while ∆ = 2 by the ﬁeld theory arguments.
On the pp-wave limit and the BMN structure of new Sasaki-Einstein spaces
In the Y p,q example we multiplied the ground state operator by one of the U (1) currents and then removed a chiral primary operator corresponding to H = 1.
On the pp-wave limit and the BMN structure of new Sasaki-Einstein spaces
In this Section we will introduce notation that will be used later in the paper and describe brieﬂy the main data-analysis techniques currently used in gravitational wave astronomy.
A template bank for gravitational waveforms from coalescing binary black holes: non-spinning binaries
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