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iGo Pitch Duo review
Posted on 29-Nov-2004 19:38
M Freitas
Filed under:
I've seen other PowerPoint solutions for handheld devices before, but the iGo Pitch Duo opens a new world of flexibility. First it supports a wide range of mobile devices, from Windows Mobile Pocket PC to Palm OS and Symbian Series 60 smartphones. Symbian users will find a copy of the QuickPoint on the software CD plus a copy of QuickWord trial, while Palm users will have a full copy of QuickOffice Pro, including applications compatible with Microsoft Word and Excel.
Users can connect handheld devices via USB using the synchronisation cables supplied with the handhelds or via Bluetooth, using the Anycom Bluetooth adapter supplied with the iGo Pitch Duo. If you decide to use the USB connection, you're welcome to use the Anycom Bluetooth adapter on your laptop or desktop, since the Bluetooth drivers are available on the software CD - although an older 1.2 version.
The iGo Pitch Duo is a small rectangular device, with two USB ports on either side of the device, and in the back we find a monitor output, plus mouse and keyboard PS/2 ports. It fits in one's hand (4.86" L x 3.05" W x 0.9" H), but despite being a very light device it is actually powered by a Pentium class CPU. This means it can get a little hot during operation, but security safeguards prevent overheating.
iGo Pitch Duo, actual size
Monitor/datashow output, mouse and keyboad ports
It supports a variety of handheld devices, but for this review we had it connected via Bluetooth with a Harrier Pocket PC Phone Edition (same as the Sprint PPC-6601, read our
Installation is simple, and following the autorun program from the CD gives us the option to install the appropriate iPresenter software for Windows Mobile Pocket PC or Palm devices, or the QuickOffice suite for Palm and Symbian devices. Palm and Symbian users can use either the iPresenter or QuickPoint to control the presentation.
The installation routine will also install a desktop converter on the host computer. This software will create a version of any Microsoft PowerPoint presentation as a sequence of slides in either .png or .jpeg formats. Of course it'll not translate neither animations nor built-in video. The file create (.pit in the Windows Mobile Pocket PC case) is then copied to the PDA. You can have as many presentations you want on your PDA, taking advantage of external storage cards for example. If you're using the QuickPoint on a Palm device you can actually edit the PowerPoint presentation on your handheld, and synchronise it both ways.
Converting a PowerPoint presentation
I've tested a 742KB presentation with both .jpeg and .png formats. The .png results are much better than the .jpeg output. The final conversion resulted in a file with 3.1MB size.
With this file we're ready to present our Microsoft PowerPoint slides from the handheld. In our case we're using a Bluetooth connection, but there's no need for pairing. We have to find what's the correct outgoing COM port used by our Bluetooth software on the Pocket PC (or Palm or Symbian devices), and instruct the iPresenter to connect from there. It'll then connect and automatically download the presentation from the PDA to the device. Tap Start and the slide sequence starts.
Finding what outgoing port my Pocket PC is using
Configuring the iPresenter software
The user interface allows the presenter to go forward and back on the slide deck, with the option of showing the slide on the monitor (or datashow), while showing the slide or comments on the Pocket PC. The slideshow preview comes in four different styles: outline view, slide view, note view or thumbnail view. The program supports 1024x768 color presentations, including VGA, sVGA, XGA.
If a mouse and keyboard are connected to the iGo Pithc Duo then these can be used to move a cursor around the screen or as an input to write comments (on the device, not on the Pocket PC of course).
The slideshow order
What you see...
...is what you get (unless you have your PDA showing other views while presenting)
On the Pocket PC the iPresenter software will allow small changes - those ones that we always do minutes before the presentation. For example you can hide slides, or change the order of the presentation. You can't actually add or change a slide, since the iPresenter is only a viewer. If you have anyone in the office able to edit the presentation and convert to the appropriate format, then this file can be sent via wireless e-mail to your device - great for connected Pocket PC (via wireless LAN or Phone Edition), Treo devices and Symbian smartphones. Of course Palm users will be able to make changes directly on their devices using the QuickPoint software supplied.
Multiple devices supported
Comes with a nice leather carrying case
Spare Bluetooth dongle
Very light
Great impression to the audience
Palm users get QuickOffice suite
Viewer software requires conversion, but no big deal
No QuickOffice version available for Pocket PC
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text: Doc ApprovedDoc Approved: Metallic Taste? Scombroid Poisoning or Carotid Dissection?Mohseni, Alex MDAuthor Information Dr. Mohseniis an emergency physician in the Washington, D.C., metropolitan area and the counsel to the president for innovation and technology of Emergency Medicine Associates. He is the editor of his own blog, Creative Health Labs. (See FastLinks.) Emergency Medicine News: January 2013 - Volume 35 - Issue 1 - p 14 doi: 10.1097/01.EEM.0000425852.89389.54 Metrics Image: ImageImage: ImageDo you remember which superficial vein thrombosis needs anticoagulation? Do you know the three different morphological patterns of Brugada syndrome? Or that the patient complaining of a new metallic taste could be having a carotid dissection? Do you recall that anal chancres from syphilis are painful while their penile cohorts are not? If the answers don't immediately come to mind, I recommend that you check out the Quick Essentials Emergency Medicine app by Deep Pocket Series, available for $16.99 on iTunes. Designed as a handy one-minute reference, it is packed with a massive amount of concise and practical information, valuable during your shift or while studying for the boards. Quick Essentials organizes its data in a way that mimics how I like to study: information is grouped in a concise, abbreviated fashion so everything is visible at once. All the different food poisoning "restaurant syndromes," for instance, are grouped in one easy-to-review table along with distinguishing features. By the way, snapper can cause ciguatera while mahi-mahi is linked to scombroid poisoning. The app struggles in its user interface. It is essentially all 222 pages of the book in sequence, and it allows users to jump to another section by choosing a different category. It has an index in the last few pages but no universal search. A resuscitation guide at the very end was important enough to include but apparently not important enough to link to in the categories. Overall, the app is a winner, and will be even more so if user interface enhancements are added. Click and Connect!Access the links in EMN by reading this issue on our website or in our iPad app, both available onwww.EM-News.com. FastLinks Read Dr. Mohseni's blog at http://CreativeHealthLabs.com. Follow him on Twitter:@amohseni. Comments about this article? Write to EMN at email@example.com. Doc APProvED is devoted to apps that can make the emergency physician's life easier, in and out of the ED. Tell us about your favorite apps by writing to Dr. Mohseni at firstname.lastname@example.com © 2013 Wolters Kluwer Health, Inc. All rights reserved.View full article text

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The Metropolitan Museum of Art, like many museums and cultural institutions, is examining its role in systemic racism and white supremacy following an outcry from staff and others about a curator's Instagram post. Officials say efforts to address race, racism and diversity in programs, staff and training at the New York City museum will be accelerated.
NYC museum grapples with diversity, systemic racism
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Hey All,
Happy Superbowl Sunday! Go Packers.
Just wanted to share the most cost efficient improvement to my system (by a country mile). I was having issues with every set of tubes that I have used in my YS Audio Symphonies Plus pre. Sovtek LP & WA, "Groovetubes" (pieces of crap), Tung Sols and my newest set of JJ 803's. My pre has a 6x4 rectifier and 3 12ax7 tubes. Nothing ever sounded as good as I had hoped and I am confident that I have had realistic expectations taking in consideration the relatively little bit of money invested in said tubes. I always experienced a little too much noise, mildly sloppy imaging, and mushy bass. Oh, and I have always used the cheap metal, springed tube covers that never seemed to lock in place very well.
So I discovered recently that there are things called "tube dampeners" which, some claimed, could improve all of my previous complaints concerning my preamp and it's tubes. I also discovered that all I had to pay was $15 for somebody's version of a tube dampener. $60 for a set of tube dampeners? Naw....I can do better than that....can't I?
I went down to Lowes and picked up 4 heavy-duty grommets from the hardware section (NOT the plumbing section) and I must say that I guessed perfectly as to which two different sizes I needed (.79 cm for the 12ax7s and .95 cm for the 6x4 rectifier).
They fit most perfectly- nice and tight without fear of cracking the tube.
So far after 1 hour there is no burning rubber smell or smoke (this is why you don't want the plumbing version of the grommet). I only put two screws into the cover just in case I needed to quickly stop my pre from going up in a blaze of glory.
Wow- tighter bass, imaging that starts to really "paint an audible picture" and much less noise. I can really crank my pre before I hear the faintest tube noise. There also seems to be less grain(?). BTW, I am coming into the pre from my new PS Audio Digilink 3 DAC which I freaking LOVE!
Highly recommended mod for those with tube equipment.


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Solvent–mediated interactions between nanoparticles at fluid interfaces
We investigate the solvent mediated interactions between nanoparticles adsorbed at a liquid–vapor interface in comparison to the solvent mediated interactions in the bulk liquid and vapor phases of a Lennard–Jones solvent. Molecular dynamics simulation data for the latter are in good agreement with results from integral equations in the reference functional approximation and a simple geometric approximation. Simulation results for the solvent mediated interactions at the interface differ markedly from the interactions of the particles in the corresponding bulk phases. We find that at short interparticle distances the interactions are considerably more repulsive than those in either bulk phase. At long interparticle distances we find evidence for a long–ranged attraction. We discuss these observations in terms of interfacial interactions, namely, the three–phase line tension that would operate at short distances, and capillary wave interactions for longer interparticle distances.
pacs:Valid PACS appear here
I Introduction
Nanoparticles can strongly adsorb at fluid interfaces, liquid–vapor or liquid–liquid Bresme and Oettel (2007). For nanoparticle sizes between 1 and 10 nm, the adsorption energy estimated from simple thermodynamics arguments Pieranski (1980) varies by several orders of magnitude, from 10 to 10 . It has been shown that the adsorption energy is very sensitive to the nanoparticle geometry Faraudo and Bresme (2003) as well as to interfacial forces such as the line tension, which can affect significantly the stability of the nanoparticles to remain adsorbed at the interface Faraudo and Bresme (2003); Aveyard and Clint (1996); Bresme and Quirke (1998, 1999a, 1999b). Moreover, it has been suggested that the coupling between nanoparticle geometry and external fields (electric, magnetic) may cause nanoparticle orientational transitions Bresme and Faraudo (2007); Bresme (2007).
The stability of nanoparticles at fluid interfaces provides a route to self assemble two–dimensional arrays and crystals, which have numerous applications in materials science Ozin and Arsenault (2005). These two–dimensional structures have also attracted the interest of condensed matter researchers, as they provide an opportunity to investigate two–dimensional phase transitions, either at equilibriumPieranski (1980); Zahn and Maret (2000); Bausch et al. (2003) or non–equilibrium conditions Zahn et al. (1997, 1999); Froltsov et al. (2003).
The interactions between nanoparticles adsorbed at fluid interfaces are expected to differ from those in the bulk. We have discussed this issue extensively in a recent review article Bresme and Oettel (2007). Nanoparticles move on a fluctuating surface that separates bulk phases (e.g. liquid and vapor), which markedly differ in their permittivities and densities. These differences in bulk properties are expected to affect the van der Waals interactions, as well as the solvent mediated interactions between particles adsorbed at interfaces. Additionally, fluctuation–induced interactions due to the soft modes of the interface capillary waves may appear, since particles adsorbed at fluid interfaces act as obstacles which modify the interfacial thermal fluctuations. This modification of the capillary wave spectrum can lead to weak long–ranged attractions Lehle et al. (2006); Lehle and Oettel (2007, 2008). Explicit Ising ferromagnet calculations in two and three dimensions have confirmed this notion, showing the existence of attractive long–ranged forces between two points pinned at an interface between two coexisting phases Abraham et al. (2007). In addition to the interface fluctuations, single nanoparticle studies suggest that the line tension can modify the wetting behavior of nanoparticles at liquid–vapor interfaces Bresme and Quirke (1998, 1999a). Whether these line tension effects are transferred to the interaction between nanoparticles is not known. The experimental investigation of this question is not easy, given the difficulties in measuring line tension effects at the nanometer scale. Experiments of nanoparticle monolayers could help to tackle these questions and could give important clues on the nature of the interactions operating between nanoparticle adsorbed at fluid interfaces Bera et al. (2007); Lin et al. (2007); Martin-Gassin et al. (2008).
In order to advance in the understanding of the nature of the interactions operating between nanoparticles at fluid interfaces, we have performed computer simulation and theoretical investigations of the solvent mediated interactions between nanoparticles adsorbed at liquid-vapor interfaces. We have modeled the nanoparticles and the solvent as a simple–liquid mixture interacting with Lennard–Jones (LJ) type potentials. The difference between the solvent–mediated interactions in the bulk phases (liquid and vapour) and those at the interface is of particular interest to us. Since solvent particles of LJ type possess a steep, repulsive core, the solvent–mediated interactions between nanoparticles with a likewise strongly repulsive core should feature the well–known depletion interactions when their surface–to–surface separation is less than a solvent diameter Israelachvili (1991). These depletion interactions play a very important role in determining the phase behavior of polymer–colloid mixtures for instance Meijer and Frenkel (1991); Lekkerkerker et al. (1992); Louis et al. (2002a). We expect they may be equally significant in tuning the interactions between nanoparticles adsorbed at fluid interfaces. Unlike the latter, the depletion interaction of hard–sphere models of nanoparticles and solvent, is very well understood using geometric concepts Oettel et al. (2009) that extend the well–known Derjaguin approximation to a more appropriate "colloidal" limit for the depletion force Botan et al. (2009). For more general solvent models of simple liquids a number of studies exist, see e.g. Refs. Shinto et al. (1999); Louis et al. (2002b); Egorov (2002); Archer et al. (2005). These results, however, are not completely understood theoretically. For larger surface–to–surface distances, i.e. away from the depletion regime, the solvent–mediated interactions between nanoparticles in bulk solvent exhibit oscillations that decay exponentially. These oscillations are connected to packing effects of the solvent particles, and consequently are more pronounced in the bulk liquid that in in the vapor phase.
In this work we show that the effective interactions between nanoparticles adsorbed at a vapor-liquid interface differ significantly from the interactions in the corresponding bulk phases. These interactions cannot be described in terms of a simple average of the two contributions (liquid and vapor). This finding applies to both the short–range depletion regime, and the regime of intermediate distances (surface–to–surface distances of up to approximately 10 solvent particle diameters). We will give a tentative interpretation of these differences as due to purely interfacial degrees of freedom, namely, the appearance of a three–phase line tension force and interfacial fluctuations.
The paper is structured as follows: In Sec. II we introduce the model and briefly describe our theoretical methods (computer simulation and reference–functional integral equations). In Sec. III we present our results for the solvent–mediated interaction between the nanoparticles in the bulk phases and at the interface. The bulk results will be interpreted using the geometrically motivated extension of the Derjaguin approximation whereas for the interpretation of the interface results we introduce the concepts of the three–phase line tension and of fluctuation–induced contributions to the solvent–mediated interactions. Sec. IV contains conclusions and an outlook.
Ii Model and methods
ii.1 Computer Simulations
Molecular Dynamics simulations in the canonical ensemble were performed for a nanoparticle pair at an explicit liquid-vapor interface. We have employed a set up similar to that used by us in previous work Bresme and Quirke (1998, 1999a, 1999b) . The solvent is modeled as a Lennard-Jones fluid,
where we use the interaction strength and the solvent diameter to define dimensionless units for the temperature , density , pressure and surface tension . The interactions between the nanoparticle and the solvent are defined in terms of the shifted Lennard–Jones potential in equation (1) Bresme and Quirke (1998),
where . We have chosen for the nanoparticle diameter. Considering a solvent diameter of about 0.3 nm, this corresponds to a nanoparticle of 2 nm, which is close to typical sizes of small metal passivated nanoparticles Heath et al. (1997); Tay and Bresme (2006). The nanoparticle-solvent interaction was set to , giving a nanoparticle–interface contact angle of 955 degrees. Because we want to isolate the solvent contributions to the interparticle interactions, the nanoparticle–nanoparticle interactions were set to zero for , i.e. beyond a hard core. All the simulations were performed for a single thermodynamic state, , where is the critical temperature of the spherically truncated and shifted Lennard-Jones model considered here Trokhymchuk and Alejandre (1999). We obtained the following coexistence densities and surface tension for this thermodynamic state: , , liquid–vapour surface tension , and pressure .
The nanoparticles were placed on the surface of a liquid slab consisting of 3 solvent atoms and dimensions . The interface plane was normal to the axis. The nanoparticles did not move during the simulations. A typical computation of the force for a specific distance involved long runs, about time steps, with a reduced time step of , which corresponds in real units to times of the order of tens of nanoseconds.
The depletion force experienced by the nanoparticles at surface–to–surface separation , is computed through,
where is the unit vector along the axis joining the centre of mass of the two particles, and , and is the force between the nanoparticle and the solvent molecules. The brackets represent an ensemble average. Similar computations were performed to obtain the potential of mean force in the bulk phases, vapor and liquid. In these cases the density of the solvent was adjusted to ensure that the density of the fluid far from the nanoparticles corresponded to the coexistence densities reported above.
In addition to the nanoparticle pair studies, we performed simulations of nanoparticle arrays at the same thermodynamic conditions. We considered a low nanoparticle surface concentration corresponding to an area per nanoparticle of , where and are the number of nanoparticles and the interface area respectively. Here, we replaced the nanoparticle hard core potential by a short range repulsive contribution,
where . The simulations involved typically 20 nanoparticles and solvent atoms. We used long trajectories, up to 10 ns, to compute the nanoparticle-nanoparticle pair correlation function, , which was later inverted to extract the total potential of mean force, ,
The solvent contribution, , can be extracted by subtracting the direct nanoparticle-nanoparticle interaction (equation (5)) from the total potential of mean force. In these simulations the nanoparticles where free to fluctuate at the interface.
We also calculated the solvent–mediated force between the nanoparticles immersed in the bulk vapor and liquid state, respectively, as well as for the two additional temperatures () and () on the isochore (i.e. away from coexistence). It is quite instructive to monitor the behaviour of the solvent–mediated force in the depletion region upon approaching coexistence (see below). Since the solvent–mediated force in the depletion region will be interpreted below in the "colloidal" limit (large nanoparticle radius), we need the nanoparticle–solvent surface tension , which can be obtained from the solvation free energy of the nanoparticle by
This definition of the surface tension is used within the integral equation approach. In order to compare the accuracy of the integral equation approach with simulation data, a different quantity is evaluated which is easier to simulate,
with chosen to be small. In the limit , the relation between both surface tensions is given by . Note that the values for and in Table I have been obtained using for the defining surface. The difference between and is small. The differences between and should become even smaller as the nanoparticle radius increases. This statement can be made quantitative by considering a simple cubic form in for the free energy of insertion,
Such a form corresponds to the well–known scaled particle picture, with representing the surface tension of a particle in the limit of infinite radius, i.e., a wall, and with , being correction terms. In the recently developed idea of morphological thermodynamics König et al. (2004), the coefficients and correspond to the free energy coefficients of the integrated mean and Gaussian curvature of the nanoparticle, and no more coefficients besides , , , are needed to describe the nanoparticle solvation free energy. The derivative of equation (9) is given by,
thus , which is formally Tolman's equation, showing that the term above decreases as . By dimensional arguments, one would expect that and , thus for larger nanoparticle radii, , we expect that and quickly converge. We note that in the limit of very small particles, with diameters a few times the solvent diameter, the main factor influencing the numerical values for the surface tension is the choice of the defining surface (see ref. Bresme and Quirke (1999a) for an illustration of this effect). Although there is some arbitrariness in this choice, it is physically reasonable to locate the surface close to the repulsive core of the nanoparticle–solvent interaction , i.e. approximately at the surface of an "exclusion" sphere around the nanoparticle. Note that for our choice we have , and for smaller values of the potential quickly rises.
ii.2 Integral Equations
The thermodynamic properties of the solvent and the solvent–mediated interaction between the nanoparticles are obtained through the pair correlation functions in the mixture of solvent particles at density with the nanoparticles at infinite dilution, . Here, species indices are '' for the solvent and '' for the nanoparticles. The first set of relations determining the correlation functions is given by the Ornstein–Zernike equations. At infinite dilution, they take the following form:
with denoting the convolution product. The second set, given by the general closure relations
requires knowledge of the bridge functions (. We employ the Reference Functional Approximation (RFA) Oettel (2005); Ayadim et al. (2009) where accurate density functionals of a hard–sphere reference system are employed to determine the bridge functions:
Here, is the reference system density functional Taylor–expanded to second order in the density deviations around the bulk densities and . Consequently, the first Taylor coefficient, the direct correlation function of first order, is a constant and given by the excess chemical potential of the reference system at bulk density : . The second Taylor coefficient is the direct correlation function of second order and depends only on the difference of the two position arguments: . As can be seen from equation (16), the bridge functions are generated from all Taylor coefficients higher than second order in an expansion of the reference free energy functional around the bulk density. The hard–sphere diameter of the reference solvent can be determined via a minimization criterion for the bulk free energy Ayadim et al. (2009), for the reference diameter for the nanoparticle we choose .
The RFA usually gives very good results for the equation of state of simple liquids, see Table I and refs. Oettel (2005); Ayadim et al. (2009), except for the immediate vicinity of critical points. Furthermore, the accuracy of fundamental measure hard–sphere functionals for highly asymmetric mixtures allows also a reliable determination of nanoparticle–solvent correlations . The effective nanoparticle–nanoparticle correlations are related to the solvent mediated potential by for . These correlation functions can be determined to good accuracy outside the depletion region () Amokrane and Malherbe (2001); Ayadim et al. (2005); Amokrane et al. (2007), inside the depletion region the "colloidal" limit expressions of refs. Oettel et al. (2009); Botan et al. (2009) can be employed (see below). The nanoparticle–solvent surface tension has been evaluated according to equation (7) by noting that the solvation free energy of the nanoparticle is the excess chemical potential in the dilute limit which within RFA is given by Oettel (2005)
By varying the nanoparticle radius, also the surface tension defined in equation (8) could be computed and compared to the corresponding values of the MD simulation (see Table I ). The agreement between simulated and integral equation results is satisfactory and underlines the usefulness of the RFA approach for very asymmetric mixtures. We verified that the cubic form for (equation (9)) constitutes an excellent fit to the RFA numerical results for nanoparticle radii between 0.5 and 10 . In these fits, the pressure which governs the volume contribution to turns out to be almost identical to the virial pressure of the solvent reported in Table I . This demonstrates the good thermodynamic consistency of RFA.
Iii Results
iii.1 Mean force of nanoparticles in bulk phases
Figure 1 shows the mean force between the nanoparticles as a function of the surface–surface separation for the bulk phases, liquid and vapor, at temperature (coexistence). The MD results for the force in the liquid phase exhibit the characteristic oscillatory behavior expected in a dense fluid, with regular peaks at intervals, and the force is attractive in the depletion region . The mean force in the vapor phase is less structured, as expected, featuring a weak repulsive force in the depletion region, indicating a preference for the nanoparticles to be solvated in the vapor phase. The mean force is determined in integral equation theory via . We find that the force between the nanoparticles in the vapor are very well reproduced by the RFA integral equation in the whole interval of distances. This is consistent with previous integral equation studies, which showed that the hypernetted chain (HNC) and Percus–Yevick (PY) integral equations very accurately reproduce the structural and thermodynamics properties of nanoparticles in bulk vapor Bresme (2002). On the other hand those studies revealed the limitations of these integral equations to predict the properties in the liquid phase. The RFA integral equation theory employed in this work shows a dramatic improvement with respect to those theories. We find that the RFA theory reproduced quantitatively the simulation results for (consistent with previous studies Amokrane and Malherbe (2001); Ayadim et al. (2005); Amokrane et al. (2007)), but fails to capture the magnitude of the attractive force in the depletion region .
The mean force between the nanoparticles in the depletion region is governed by the density distribution of the solvent spheres in the annular wedge formed between the nanoparticles. With the radius of the nanoparticle becoming large, the annular wedge induces a quasi–two dimensional confinement for the solvent spheres. Bulk integral equations (as employed here) do not capture this regime well. Explicit density functional studies for hard spheres and large nanoparticle radii Botan et al. (2009) suggest the validity of the following expression for the depletion force in the "colloidal" limit (large nanoparticle radius):
Here, is an effective radius of the nanoparticle (i.e. an equipotential surface). For hard spheres, the obvious choice would be , the radius of the exclusion sphere around the nanoparticle. The above expression for the depletion force follows only from geometric considerations on the overlap region of the two exclusion spheres Oettel et al. (2009); Botan et al. (2009). Let , and denote the volume, surface area and integrated mean curvature of this overlap region (which obviously depend on the distance between the centers of the exclusion spheres). According to morphological thermodynamics König et al. (2004) which we already briefly introduced in the discussion of the solvation free energy of one nanoparticle (equation (9)), the depletion potential takes the form , where is the pressure in the solvent, is the nanoparticle–solvent surface tension and is the mean curvature coefficient. The mean force follows as . Note that with , equation (20) turns into the well–known Derjaguin approximation for the mean force which is widely employed in colloidal physics. The coefficient can actually be interpreted as a line tension associated with the edge of the annular wedge between the nanoparticles Oettel (2004). Obviously, this line tension becomes important either when in equation (20) or if both and are numerically small.
We have tested this form for the mean force on the isochore for the temperatures (coexistence), 1.0 and 1.25 (see Table I ). In applying equation (20), we have used as one would do for hard spheres and we employed the surface tension from the RFA at the respective state points (see Table I ). For the coefficient , we used the value which has been determined by a fit to the simulation results for the depletion force at and which we use also for the other temperatures.111In principle, can be detemined from the insertion free energy of a single nanoparticle with varying radius and thus should be equivalent to the –coefficient appearing in equation (9). However, it is not clear how the nanoparticle–solvent potential must be chosen for different such that the coefficient is unequivocally determined. This is yet an open question in the application of morphological thermodynamics to soft potentials. In Figure 2 the MD data (symbols) are compared to the theoretical expressions (full lines) and the Derjaguin approximation (, dashed lines). It can be seen that the Derjaguin approximation is almost on top of the data points for , the state point deep in the liquid but it fails to catch the upturn of the force for for the two lower temperatures. The line tension term indeed can account for this behaviour. It is even the dominant term for the state point right at coexistence where both the reduced pressure (RFA) and the reduced surface tension (RFA) are numerically small, as anticipated before.
iii.2 Mean force of nanoparticles at the liquid-vapor interface
Figure 3 represents the main result of this paper. We report the solvation force between nanoparticles adsorbed at the liquid–vapor interface. We recall that the solvent–nanoparticle interactions used in our simulations result in a nanoparticle contact angle slightly larger than 90 degrees, showing there is not a strong preference for the nanoparticles to be immersed in the vapor or liquid phases. Comparison of the force between the nanoparticles at the interface (circles in Figure 3) with the vapor (diamonds in Figure 3) and liquid (squares in Figure 3) counterparts shows that there is not a trivial relationship between the forces at interfaces and in the bulk. This is particularly evident in the depletion region, , where the interaction between the nanoparticles at the interface is considerably more repulsive than in the bulk phases. The repulsive force, , amounts to about 8 pN, considering the standard Lennard-Jones parameters for Argon ( kJ/mol, Å). Therefore, the simple geometric description leading to equation (20) for the force is not valid for the interface case, since it would lead to a weighted superposition of the liquid and vapour forces and thus to an almost zero force in the depletion region. The main conclusion from the data represented in Figure 3 is that the interface adds a contribution to the force that is not present in bulk. One possible origin for this force could be again a line tension. For nanoparticle separations corresponding to the depletion region, , there exists a three phase line surrounding the nanoparticle pair. The three phase line will tend to contract for positive line tensions and expand for negative ones, adding an attractive or repulsive contribution respectively, to the total force between the nanoparticles. A repulsive force like the one we observe in our simulations would indicate a negative line tension. We have made an attempt to estimate the order of magnitude of the line tension needed to generate a repulsive force of the order of the one observed in the computer simulations. To this end we consider a phenomenological model, whereby the line tension contribution to the free energy is given by, , where is the length of the three phase line surrounding the nanoparticle pair (cf. Figure 4). Hence, within this model the force due to the line tension, assuming a nanoparticle contact angle of 90 degrees is given by:
This contribution is very similar to the line tension contribution in equation (20) for the depletion force in the bulk. is the radius defining the three phase line (see Figure 4). A natural choice for this radius would be , as before, but one could equally well choose a somewhat larger value (e.g., where the nanoparticle–solvent potential is minimal). Because at this molecular scale it is difficult to split up the force contributions due to part of the nanoparticle being in the vapor phase and other part in the liquid phase, we can only attempt to estimate the sign and order of magnitude of the line tension. Considering equation (III.2), the magnitude of the force when the nanoparticles are in contact (), and , we estimate a line tension of the order of . The order of magnitude and sign of the line tension obtained from this analysis is similar to the values reported from computations of nanoparticles adsorbed at Lennard–Jones liquid–vapor interfaces, where line tensions of the order of were found Bresme and Quirke (1998, 1999a).
To further test the existence of the extra repulsive contribution between the nanoparticles in the depletion region, we have performed simulations of nanoparticle arrays adsorbed at the liquid-vapor interface (see section II.1 for details). Figure 5 shows the corresponding potentials of mean force (PMF), which were obtained from integration of the forces for the nanoparticle pair, and from inversion of the pair correlation function (equation (6)) for the nanoparticle array. The agreement between both computations in the depletion region is excellent, showing that the PMF obtained from the nanoparticle pair represents an accurate approximation for the short range interactions between particles at the low coverages investigated in this work. Comparison of the PMF at the interface with the bulk phases (c.f. Figure 5) makes even clearer the strong impact that the interface has on the nanoparticle interactions.
Finally, we discuss the long range behavior of the potential of mean force between nanoparticles at the liquid–vapor interface (c.f. Figure 6). For the purpose of analyzing the decay of the interactions in the bulk phases we have considered the integral equation results. We showed above that the RFA integral equation provides an excellent approximation to the simulation results. The potential of mean force for the bulk phases, liquid and vapor, decays to zero for nanoparticle separations being of the order of 6, whereas it shows a longer–ranged behavior in the case of nanoparticles adsorbed at the interface. (Note that in the integration of the MD force data at the interface, we have set the potential to zero for the longest distance investigated in this work (10)). The occurence of a long–ranged tail in the PMF at the interface might be connected with capillary waves. It has been suggested that colloids adsorbed at fluid interfaces act as obstacles which perturb the fluctuations of the capillary waves through boundary conditions at the three phase contact line Lehle et al. (2006). For colloids placed at the interface at center–to–center distance , the fluctuation spectrum and consequently the free energy of the capillary waves will depend on . This results in a distance–dependent fluctuation force, which has been described as a variant of the Casimir force (originally thought of as induced by quantum fluctuations). It has been shown that the fluctuation force is strongly dependent on the boundary conditions applying to the colloids, namely, whether the colloids are fixed or fluctuate. For fixed colloids like the ones investigated here and a freely fluctuating three–phase contact line, the fluctuation force in the limit of the capillary length is given by Lehle et al. (2006); Lehle and Oettel (2007, 2008),
This equation was derived in the context of a structureless solvent, where the spectrum of the interface position fluctuation is entirely governed by the capillary wave hamiltonian Buff et al. (1965)). Thereby molecular effects are ignored. We expect that equation (22) will become a good approximation for long interparticle distances, since in this case the molecular nature of the solvent becomes secondary with respect to the fluctuations of the interface. Nonetheless, it is difficult to quantify the distance at which molecular effects become unimportant. This distance can be estimated considering the results reported in a very recent work. It has been shown that the dynamics of nanoscopic capillary waves on Lennard–Jones liquid surfaces shows very good agreement with the hydrodynamic theory down to very small wavelengths, of about four molecular diameters Delgado-Buscalioni et al. (2008). This result indicates that a continuum approximation may provide an accurate approach at very small length scales.
We note that the finite size of our simulation box sets a cutoff for the capillary wave spectrum. Hence, equation (22) can not be used directly. The full leading term in for a finite capillary length in an expansion in is given by Lehle and Oettel (2007, 2008)
where . In Figure 6 we show the predicted fluctuation force for a capillary length which corresponds roughly to half the lateral box size used in the simulations and is thus intuitively the correct cutoff for the capillary waves. (Note that also has been set to zero at which corresponds to ). We find that this force has an order of magnitude and decay that agrees well with the simulation results, indicating that capillary fluctuations could add a non negligible contribution to the interactions between nanoparticles at long separations. The small magnitude of is also due to the smallness of the capillary length; for a realistic capillary length of about 1 mm, the fluctuation–induced potential increases by a factor 4 …5 in the distance regime shown in Figure 6.
Iv Summary and final remarks
We have reported computer simulations and integral equation studies of the interactions between a nanoparticle pair immersed in bulk liquid or vapor and adsorbed at the liquid–vapor interface of a simple liquid. We have considered a situation in which the nanoparticles have a contact angle of the order of 90, hence they do not show a strong preference for the vapor or the liquid phase.
The potential of mean force for the nanoparticles in the bulk phases can be explained well by a combination of geometric arguments for the depletion region (where the surface–to–surface separation of the nanoparticles is less than one solvent diameter) and of reference functional integral equations for larger separations. We have found that the potential of mean force between the nanoparticles adsorbed at the interface is significantly different from that obtained in the liquid and vapor phases. The interactions at the interface cannot be explained as a simple average of the interactions in the corresponding bulk phases. Specifically, in the depletion region the nanoparticles repel each other more strongly than in any of the bulk phases. This repulsive interaction is of the order of 2–3 at zero nanoparticle separation. We have confirmed the existence of this repulsive interaction using computer simulations of low density nanoparticle monolayers adsorbed at the liquid–vapor interface, where the potential of mean force can be alternatively obtained from inversion of the nanoparticle–nanoparticle pair correlation function.
Our analysis suggests that the line tension associated to the three phase line surrounding the nanoparticle pair may add a significant contribution to the nanoparticle interactions in the depletion region. We have estimated that the line tension needed to induce a repulsive force of the order of the one observed in the simulations is negative and of the order of N. This order of magnitude and sign agrees with the line tensions estimated in previous investigations of nanoparticles adsorbed at liquid–vapor interfaces Bresme and Quirke (1998, 1999a). We have also shown that the interactions between the nanoparticles immersed in the bulk phases (vapor and liquid) decay to zero within about six solvent molecular diameters, whereas the interaction between nanoparticles at the liquid–vapor interface features a longer range attraction that appears to extend beyond ten solvent molecular diameters. The magnitude and decay of the attractive potential is of the order predicted from a theoretical analysis of the force arising from the perturbation of the interfacial capillary fluctuations Lehle et al. (2006); Lehle and Oettel (2007). Our work suggests that interfacial (line tensions and capillary waves) degrees of freedom may add a non negligible contribution to the depletion forces between nanoparticles at interfaces. Overall, our model of nanoparticles adsorbed at realistic liquid–vapor interfaces indicate that the depletion force contributes with 1–2 to the total interaction between nanoparticles at interfaces.
Acknowledgements.FB would like to thank The Royal Society for financial support and the Imperial College High Performance Computing Service for providing computational resources. MO thanks the German Science Foundation (DFG) for financial support through the Collaborative Research Centre (SFB–TR6) "Colloids in External Fields", project N01.
- Bresme and Oettel (2007) F. Bresme and M. Oettel, J. Phys.: Condens. Matt. 19, 413101 (2007).
- Pieranski (1980) P. Pieranski, Phys. Rev. Lett. 45, 569 (1980).
- Faraudo and Bresme (2003) J. Faraudo and F. Bresme, J. Chem. Phys. 118, 6518 (2003).
- Aveyard and Clint (1996) R. Aveyard and J. Clint, J. Chem. Soc. Faraday Trans. 92, 85 (1996).
- Bresme and Quirke (1998) F. Bresme and N. Quirke, Phys. Rev. Lett. 80, 3791 (1998).
- Bresme and Quirke (1999a) F. Bresme and N. Quirke, J. Chem. Phys. 110, 3536 (1999a).
- Bresme and Quirke (1999b) F. Bresme and N. Quirke, Phys. Chem. Chem. Phys. 1, 2149 (1999b).
- Bresme and Faraudo (2007) F. Bresme and J. Faraudo, J. Phys.: Condens. Matter 19, 375110 (2007).
- Bresme (2007) F. Bresme, Eur. Phys. J. B 64, 487 (2007).
- Ozin and Arsenault (2005) G. Ozin and A. Arsenault, Nanochemistry: A Chemical Approach to Nanomaterials, RSC Publishing, Cambridge (2005).
- Zahn and Maret (2000) K. Zahn and G. Maret, Phys. Rev. Lett. 85, 3656 (2000).
- Bausch et al. (2003) A. R. Bausch, M. J. Bowick, A. Cacciuto, A. D. Dinsmore, M. F. Hsu, D. R. Nelson, M. G. Nikolaides, A. Travesset, and D. A. Weitz, Science 299, 1716 (2003).
- Zahn et al. (1997) K. Zahn, J. Mendez-Alcaraz, and G. Maret, Phys. Rev. Lett. 79, 175 (1997).
- Zahn et al. (1999) K. Zahn, R. Lenke, and G. Maret, Phys. Rev. Lett. 82, 2721 (1999).
- Froltsov et al. (2003) V. Froltsov, R. Blaak, C. Likos, and H. Löwen, Phys. Rev. E 68, 061406 (2003).
- Lehle et al. (2006) H. Lehle, M. Oettel, and S. Dietrich, EPL 75, 174 (2006).
- Lehle and Oettel (2007) H. Lehle and M. Oettel, Phys. Rev. E 75, 011602 (2007).
- Lehle and Oettel (2008) H. Lehle and M. Oettel, J. Phys.: Condens. Matter 20, 404224 (2008).
- Abraham et al. (2007) D. Abraham, F. Essler, and A. Maciolek, Phys. Rev. Lett. 98, 170602 (2007).
- Bera et al. (2007) M. Bera, M. Sanyal, S. Pal, J. Daillant, A. Datta, G. Kulkarni, D. Luzet, and O. Konokalov, Europhys. Lett. 78, 56003 (2007).
- Lin et al. (2007) B. Lin, D. Schultz, X.-M. Lin, D. Li, J. Gebhardt, M. Meron, and P. Viccaro, Thin Solid Films 515, 5669 (2007).
- Martin-Gassin et al. (2008) G. Martin-Gassin, Y. El-Harfouch, E. Benichou, G. Bachelier, I. Russier-Antoine, C. Jonin, S. Roux, O. Tillement, and P.-F. Brevet, J. Phys.: Condens. Matter 20, 055228 (2008).
- Israelachvili (1991) J. Israelachvili, Intermolecular and Surface Forces (Academic Press, London, 1991), 2nd ed.
- Meijer and Frenkel (1991) E. Meijer and D. Frenkel, Phys. Rev. Lett. 67, 1110 (1991).
- Lekkerkerker et al. (1992) H. Lekkerkerker, W. Poon, P. Pusey, A. Stroobants, and P. Warren, Europhys. Lett. 20, 559 (1992).
- Louis et al. (2002a) A. Louis, P. Bolhuis, E. Meijer, and J. Hansen, J. Chem. Phys. 117, 1893 (2002a).
- Oettel et al. (2009) M. Oettel, H. Hansen-Goos, P. Bryk, and R. Roth, EPL 85, 36003 (2009).
- Botan et al. (2009) V. Botan, F. Pesth, T. Schilling, and M. Oettel, preprint (2009).
- Shinto et al. (1999) H. Shinto, M. Miyahara, and K. Higashitani, J. Colloid Interface Sci. 209, 79 (1999).
- Louis et al. (2002b) A. Louis, E. Allahyarov, H. Löwen, and R. Roth, Phys. Rev. E 65, 061407 (2002b).
- Egorov (2002) S. Egorov, Phys. Rev. E 70, 031402 (2002).
- Archer et al. (2005) A. Archer, R. Evans, R. Roth, and M. Oettel, J. Chem. Phys. 122, 084513 (2005).
- Heath et al. (1997) J. Heath, C. Knobler, and D. Leff, J. Chem. Phys. 101, 189 (1997).
- Tay and Bresme (2006) K. Tay and F. Bresme, J. Am. Chem. Soc. 128, 14166 (2006).
- Trokhymchuk and Alejandre (1999) A. Trokhymchuk and J. Alejandre, J. Chem. Phys. 111, 8510 (1999).
- König et al. (2004) P. König, R. Roth, and K. Mecke, Phys. Rev. Lett. 93, 160601 (2004).
- Oettel (2005) M. Oettel, J. Phys.: Condens. Matter 17, 429 (2005).
- Ayadim et al. (2009) A. Ayadim, M. Oettel, and S. Amokrane, J. Phys.: Condens. Matter 21, 115103 (2009).
- Amokrane and Malherbe (2001) S. Amokrane and J. Malherbe, J. Phys.: Condens. Matter 13, 7199 (2001).
- Ayadim et al. (2005) A. Ayadim, J. Malherbe, and S. Amokrane, J. Chem. Phys. 122, 234908 (2005).
- Amokrane et al. (2007) S. Amokrane, A. Ayadim, and J. Malherbe, J. Phys. Chem. C 111, 15982 (2007).
- Bresme (2002) F. Bresme, J. Phys. Chem. B 106, 7852 (2002).
- Oettel (2004) M. Oettel, Phys. Rev. E 69, 041404 (2004).
- Buff et al. (1965) F. P. Buff, R. A. Lovett, and F. H. Stillinger, Phys. Rev. Lett. 15, 621 (1965).
- Delgado-Buscalioni et al. (2008) R. Delgado-Buscalioni, E. Chacón, and P. Tarazona, Phys. Rev. Lett. 101, 106102 (2008).


text:
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HOOKER: L J: address, phone, fax, email, site
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HOOKER: L J is Australian proprietary company. This firm was registered on 2011-04-25 and was issued with the 352465820 ACN. Its Australian Business Number is 21848754861. Since 2011-04-25, the company is headquartered in Australia. The previous headquarters were located in 1ST FLOOR, SUITE 5, 6 SOMERSET AVE NARELLAN 2567. HOOKER: L J was registered for the GST on 2011-04-25. In total the company used 1 trading name. Category of HOOKER: L J is a . We found 0 trademarks that mention this company.
Company HOOKER: L J was registered in 2011-04-25 in AU, full name of company is HOOKER: L J. The company HOOKER: L J is located on the address: 1ST FLOOR, SUITE 5, 6 SOMERSET AVE NARELLAN 2567. We bring you a complete range of reports and documents featuring legal and financial data, facts, analysis and official information from The Main AU Registry. Less 10 employees work in the company. Capital of company is 676,000 AUD, sales per year is Less 821,000,000 AUD, credit rating of HOOKER: L J is Normal. HOOKER: L J is Foreign. Company has the Australian Company Number (ACN) as 352465820 and Australian Business Number (ABN) as 21848754861.
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Mobile apps have become an important part of businesses now. The increased use of these mobile apps among users these days has prompted businesses worldwide to invest their time in creating responsive mobile apps suiting their business specifics.
In the year 2018, global mobile app revenues amounted to over 365 billion U.S. dollars. In 2023, it is expected that mobile apps would generate a revenue of more than 935 billion U.S. dollars through paid downloads and in-app advertising, says Statista.
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Operating System Platform!
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In the third quarter of 2019, Android users have approximately 2.47 million apps to choose from Google Play store, while Apple App Store is the second-largest app store offering 1.8 million iOS apps, says Statista.
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Carefully going through the company website is one of the most important things to consider before hiring a mobile app development company. Before you choose a mobile app development company to build a mobile app, you should have a look at its website. This helps you to know what kind of services they offer.
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I am sure you certainly don't want this to happen with your business's website. These days almost all mobile development companies have a business website. A well-designed small business website is the best way of making a long-lasting impression on the target audience. Do an exhaustive research about the company by meticulously going through its website and find out for how many years they have been into the business. Choose the one that has around 3-4 years of experience in the industry.
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Next in the list of factors to consider before hiring a company is having a look at the past work done and the stages of mobile app development executed by the company for developing mobile apps. To know about the company's past work, you just need to land on the portfolio page and see what type of projects they have worked on in the past. Get all the details of the mobile applications the company has made so far. Download the same type of apps from respective app stores to know about all the features of the app in detail.
Let's say for instance, if you are planning to build a banking app, then before hiring the company for developing the app, it's important to find out whether the company has prior experience in building similar apps in the past. Get detailed information about the app that's there on the portfolio page and know about its features. You can also download the app and then see how it functions.
[Read: Building A Mobile App For Your Business? Consider These 12 Factors First!]
Client Testimonials!
Here is more on what to consider while hiring a mobile app development company. Let's read further in detail about the important things to consider before hiring a mobile app development company. Before you hire a mobile app development company, you must read the client testimonials on their website. This helps you to view all the reviews, feedback, and comments provided by the clients who have hired the company in the past.
4% of consumers say that positive reviews help them in making their buying decision and allow them to trust a local business more. For every increase of one-star in a Yelp rating means a 5 to 9% increase in revenue.
You can also ask for some past or current client references to check the reliability of the company. You can also contact these clients via email or phone number to get their feedback on the services offered by the company.
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Eileen Carey's goal 40 seconds into overtime was a true Valentine's Day gift to her team. Carey's score gave the University School co-op a 4-3 victory over the Onalaska Hilltoppers in a non-conference girls' hockey game on Friday, February 14th at the Omni Center in Onalaska.
Carey took a pass from Jordan Bonk as she, Bonk, and Emily Mueller entered the Onalaska zone on a three-on-two break. Carey described her game-winning goal. "When Jordan, Emily, and I skated down open ice, I wasn't really expecting the pass, more likely a shot on goal or possibly a rebound. When the puck hit my stick, it felt like it was on my stick forever. I finally got it off my stick and didn't even see where it went in. But as long as it hit the net, I'm happy with it. I've never experienced a better feeling. The girls worked hard tonight, and I definitely feel like the win was well deserved."
Bonk, who is a captain of the Wildcats, added, "The win today felt great. I feel like we really deserved this tonight, and it was a great way to start off this weekend. My assist on the overtime goal all happened because I had confidence that Eileen could put the puck in the net. Overall, it was a great game to come off of into our next game and then sectionals."
As both players implied, the Wildcats took the action to their hosts in the annual end of the season contest between these two teams. They outshot the Hilltoppers 26-18. Sami Stommel, USM's goaltender, made 15 saves in the game. Izzy Lassa, Onalaska's goalie, made 22 saves.
The Wildcats began aggressively, taking 12 shots in the game's first period and scoring on one of them. Zoe Uihlein, who was playing forward instead of her usual position defense, scored the night's first goal. From the slot, she backhanded a rebound of a shot by Zoe Neudorfer past Lassa at 13:41.
Onalaska tied the score on a power play with just 7 seconds left in the opening period. Tessa Deal skated the puck into the Wildcats' left corner where she was met by a defender. Mac Seiler joined her and pulled the puck free from the scrum. Seiler centered it. Jaidyn Groshek swiped at it. The puck caromed off her stick, fluttered into the air, and fell behind Stommel to make it 1-1 at the end of the period.
The Wildcats scored the only two goals in the second period. Forechecking in the Hilltoppers' right corner, Rachel Gauthier stopped a defenseman. Molly Guenther got the loose puck and zipped a pass toward the crease. Neudorfer was standing at the near post, and she swatted the puck between Issa's pad and the pipe at 7:58.
Uihlein scored her second goal of the game just over a minute later. Mallory DeLuca halted an Onalaska clearing attempt along the left boards at the Onalaska blue line. Uihlein grabbed the puck and whipped it down the boards to the corner. Neudorfer collected it and headed behind the net. Before she got there, she backhanded the puck out front to Uihlein who snapped it into the net, giving the Wildcats a 3-1 lead at 9:01.
The Hilltoppers were down but not out. They tied the score with two goals in the third period. Jaden Hammes scored both of them. She scored the first of them at 3:56 of the period. Skating out of the Onalaska end, Deal fired a cross ice pass toward the Wildcats' blue line. The puck hit a defenseman's stick and skittered to the left boards. Hammes scooped it up, skated to the edge of the circle, and blazed a shot past Stommel.
Hammes tied the score on a similar play late in the period. She snared a loose puck along the left boards in center ice and took off. She sped past a tripping defenseman and went in on a breakaway. From the left circle she gunned a shot into the net at 14:01.
That goal set up an overtime period. It wasn't a long one. Carey made sure of that with 7:20 left in the added eight minutes.
After the game, Uihlein, who is also a captain of the Wildcats, said, "Today's game was a great way to start off the weekend. We really worked hard as a team to get that win. As a defenseman moving up to forward for a game, I wasn't expecting at all to get those two goals, but it was all thanks to my teammates for their great passes to me in the slot."
Onalaska's record is 12-10. The Hilltoppers play the penultimate game of their season when they host Hudson at the Omni Center at 7:00 p.m. on Saturday, February 15th.
As a result of the win, USM is now 6-13-4. The Wildcats finish their regular season play in the second game of their swing through southwestern Wisconsin. They face off with Black River Falls in a non-conference game at noon on Saturday, February 15th at the Mose Lamb Hockey Rink in Tomah.
Tag(s): Home Game Summaries Girls Varsity Eastern Shores USM Wildcats Independents Onalaska


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How to Become a Major
The undergraduate program in Art History welcomes students seeking to become Art History majors both as a stand-alone degree and as a double major, for example with a B.F.A. in a studio concentration or the B.F.A. in Visual Art Studies. In order to become an Art History major, you need to:
- Be accepted as a student in the College of Visual Arts and Design. Check out our Admissions page for more information about how to apply.
- Email the Department Student Coordinator at firstname.lastname@example.com to discuss completing your degree plan.
- Go to the Registrar's Office, located in the ESSC, and request a copy of all your transcripts to submit to the department with your degree plan. Your degree plan cannot be completed without these transcripts.
That's it! And you can declare your major in Art History as early as your first semester at UNT.
If you have questions about the process, feel free to contact the Department of Art Education and Art History at email@example.com.


text:
@MISC{Mitra_artificialimmune, author = {Pinaki Mitra and Ganesh K. Venayagamoorthy}, title = {Artificial Immune System Based DSTATCOM Control for an Electric Ship Power System}, year = {}}
is a shunt compensation device which is generally used to solve power quality problems in distribution systems. In an all-electric ship power system, these power quality problems mainly arise due to the pulsed loads, which causes the degradation of the entire system performance. This paper presents the application of DSTATCOM to improve the power quality in a ship power system during and after pulsed loads. The control strategy of the DSTATCOM plays an important role in maintaining the voltage at the point of common coupling. A novel adaptive control strategy for the DSTATCOM based on artificial immune system (AIS) is proposed. The optimal parameters of the controller are first found using particle swarm optimization. This provides a sort of innate immunity to common system disturbances. For unusual system disturbances, these optimal parameters are modified online, thus providing adaptive immunity in the control system. To evaluate the performance of the DSTATCOM and the AIS adaptive controller, a ship power system is developed in the MATLAB/SIMULINK environment. The effectiveness of the DSTATCOM and the AIS controller is examined for pulsed loads of different magnitudes and durations. I.
artificial immune system
dstatcom control
electric ship power system
power quality problem
ship power system
pulsed load
optimal parameter
important role
control system
shunt compensation device
novel adaptive control strategy
common system disturbance
entire system performance
particle swarm optimization
all-electric ship power system
unusual system disturbance
ai adaptive controller
ai controller
power quality
common coupling
adaptive immunity
different magnitude
innate immunity
control strategy
distribution system
matlab simulink environment
Developed at and hosted by The College of Information Sciences and Technology
© 2007-2019 The Pennsylvania State University


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Ushaw College Swimming Bath
Photo of Swimming Baths Ushaw College.
Anyone remember this ? Was it available for anyone to use or just the Students of the College ?
August 10, 2011 at 12:39 pm
I used to go to St. Joseph's RC School in Ushaw Moor and once a year we would be taken to Ushaw College and could use the pool. It was only available for College Students/Staff. I can't make it out clearly on the photo but there used to be small individual changing cubicles around the outside of the pool (late 1980's).
August 11, 2011 at 1:41 pm
The Swimming Baths were still there and in daily use about 10/15 years ago. My eldest brother Jim was a joiner at Ushaw College and the first time I went up to the College after I retired he showed me around and a visit to the Baths was on the tour.
When I used to roam the beck as a young lad there was a small pump house in working order about 200 yards up the beck in the direction of Broadgate on the right hand bank from what we knew as "The Plank". There is a small bridge across the beck now in place of "The Plank" at the bottom of the path that leads down from Deerness View. Where the water was pumped to I do not know but the crack was that it was pumped to Ushaw College Baths. I doubt that now as the water was not exactly the cleanest. There was always a very small leak from an external pipe leading into the pump house and the water froze in winter and formed an arch of ice about 4/5 feet in length, very thin and very fragile.
A few yards away from the pump house there was a large man made basin dug out of the earth. Grass grew on the floor and side of the basin and whatever its original use it was even then many years since it was used for its original purpose. The crack then that this was used as a swimming pool by the College students before the Baths were built at Ushaw. Whether there was any truth in that explanation I do not know.
A few yards up stream there was and still is a weir built across the beck. I never knew the reason for the weir being built there. This is a hundred yards downstream from the crossing at Broadgate. Can anyone shine any light on this question.
In the same area and just yards downstream from the crossing at Broadgate someone told me that a lot of years ago there was a small factory that produced bricks and tiles. Again I wonder if anyone can shine any light on this.
Brian Mc.
November 27, 2011 at 5:36 pm
I swam in that pool…possibly sometime in the 70's…. the coldest water I ever had the privilege of diving in…!!! thanks for the photo….
February 7, 2012 at 12:28 am
could anyone give me the location of this, i heard that the building is there but I'm unsure of the location and i would like to go explore and take some photos


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Difference between revisions of "The Team 2 Down Current Issues As Well As Blackouts"
(Created page with "Our brand-new GeForce Video game Ready driver is maximized for The Staff 2. To download as well as install, merely discharge up GeForce Experience and click the "Drivers&...")
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Latest revision as of 09:16, 1 July 2020
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