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Grids / Fixed Rows on Top and Bottom Side
This example shows how to fix rows on top and bottom side in TreeGrid directive. By right-clicking some row in the TreeGrid, a context menu will popup showing fixed position: top, bottom or none. By selecting a menu option, the TreeGrid layout will update showing fixed rows.
Each row object has a field which allows you to set the side at which it will be fixed.
- fixed - Determines the side at which row will be fixed. This field accepts one of the following values: 'none', 'top' or 'bottom'.
When row is fixed, it cannot expand/collapse, selection is suppressed and also drag drop operations are excluded. If fixed row has child rows, they are excluded from TreeGrid layout. Scrolling is also updated so that only non-fixed rows can be scrolled.
You can customize the appearance of fixed colurowsmns by using corresponding CSS styles. You can find more information in code of this sample.


CordovaLib is a static library that enables users to include Cordova in their iOS application projects easily, and also create new Cordova based iOS application projects.
Make sure you have installed the latest released iOS SDK which comes with Xcode 4. Download it at http://developer.apple.com/ios.
You don’t need to do this if you downloaded the installer from http://incubator.apache.org/cordova/, this is only for developers that need to compile the source.
The installer should build “CordovaInstaller.dmg” into the dist folder, mount the .dmg, then:
NOTE: For 2.0.0, the use of Xcode Templates has been removed. If you don’t plan on using older Cordova versions, you should run the uninstaller first.
The docs should also have been included in the distribution.
NOTE: For 2.0.0, the use of Xcode Templates has been removed. If you don’t plan on using older Cordova versions, you should run the uninstaller first.
Use the “Uninstall Cordova” app included in the Cordova iOS DMG file, OR:
NOTE:
It will ask you to confirm whether you want to delete the installed CordovaLib directory (just in case you made changes there) as well as the Cordova framework. It will not ask for confirmation in deleting the installed Xcode templates.
This installer will only install items under your home folder (signified by ~)
Items that will be installed:
To uninstall:
Delete the files listed above, or use the “Uninstall Cordova” app included in the Cordova iOS DMG file.
1. In Xcode 4 (for Cordova versions lesser than 2.0.0) , I get an error that “The Start Page ‘www/index.html’ was not found.”?
This is a known issue with the Xcode 4 Template - we can’t specify a folder reference. You need to build the project at least once, then go to the folder where your project is in, and drag and drop in the www folder, then add it as a folder reference (will end up as a blue folder, not yellow), then run the project again. Check your project warnings as well for clues.
2. When I run the Installer, the installation fails?
Usually it’s a folder permissions issue with the templates folder, changed by other third-party installers. You can trouble-shoot using the instructions here.
3. When I add Plugins, they are not found or won’t compile?
Check your Xcode Console Log for clues.
This can be because of:
4. I get this error in my Xcode Console Log - ‘ERROR whitelist rejection: url=’http://<MYHOSTNAME>/’
This error occurs because of the new white-list feature in version 1.1.
You will have to add any hosts your app uses or connects to (hostnames/IP addresses only, without the protocol nor the path) in Cordova.plist/ExternalHosts. Wildcards are supported.
This includes external http/https/ftp/ftps links in:
5. How do I effectively upgrade my project?
Starting with Cordova 1.4, follow the instructions in the “Upgrading Cordova iOS” document.
6. I’ve got ‘symbol not found’ errors during runtime? Usually it’s because I’m deploying to an iOS 3.x device.
With version 0.9.6, we implemented the W3C Media Capture API, which requires use of some iOS 4 APIs and frameworks. If you are deploying to an iOS 3.x device, you will need to “weak/optional” link three frameworks: UIKit, CoreMedia, and AVFoundation.
If you get a “Symbol not found: NSConcreteGlobalBlock”, you will have to weak link libSystem through a command-line option.
This is because the LLVM compiler strong links NSConcreteGlobalBlock, but gcc weak links (correctly). Add a linker flag in “Other Linker Flags” in your project target: “-weak-lSystem”
Starting with version 1.1, when creating a new project, the weak-linking is added through a linker flag so you will not need to do this manually.
7. How do I override the location of the start page www/index.html?
Starting with Cordova 1.4, you can set this directly in the function application:didFinishLaunchingWithOptions: in your project’s AppDelegate.m file.
Modify these lines appropriately:
8. What’s the difference between the two templates?
Note that Xcode template support has been removed in 2.0.0.
The CordovaLib static library is only used by the older subproject-based template. The Xcode 4 template uses Cordova.framework (a static framework) because of Xcode 4’s template limitations. Both are based off the same code, just packaged differently.
Staring with 2.0.0, you must create projects using the command line:
9. In the sub-project based Cordova project, I want to have a project-specific copy of CordovaLib for my project, not a global one. How do I do this?
In your project, there should be a CordovaBuildSettings.xcconfig file. Modify the CORDOVALIB variable in the file to point to your project specific CordovaLib folder. You can use relative paths, off $(PROJECT_DIR).
10. In a .framework based Cordova project (only supported in Cordova versions lesser than 2.0.0), I want to have a project-specific copy of Cordova.framework for my project, not a global one. How do I do this?
Remove the existing Cordova.framework from your project, and drag and drop your own Cordova.framework in, that’s all there is to it. To compile your own version of Cordova.framework, go to ~/Documents/CordovaLib and run the Xcode project with the UniversalFramework target. You might need to modify the USER_FRAMEWORK_SEARCH_PATHS in your project as well.
11. I’ve got other Cordova-specific issues not covered here?
Do a search in the Apache JIRA Issue Tracker Apache JIRA or the Wiki.
12. On an iOS 3.2 iPad, and launching an iPhone only app, when I use the Media Capture API, the user interface shown is iPad sized, not iPhone sized?
You must delete the ~ipad.png images from Capture.bundle if they want to build an iPhone only app and have captureAudio() display properly on an iPad. This additional fix is just for iPad running iOS 3.2 - if the requested ~ipad.png is not available it returns the iPhone sized image.
13. I get this linker error: “ld: warning: ignoring file libCordova.a, file was built for archive which is not the architecture being linked (armv7)”
In your project’s Build Settings, set “Build for Active Architecture Only” to NO. This has been fixed in Cordova 1.2 for newly created projects. This is usually because Xcode 4 will only build for armv7 by default, and not armv6.
14. I get this runtime error/crash: “dyld: Symbol not found: _NSURLIsExcludedFromBackupKey”
A. Older iOS versions than 5.1 do not have this symbol defined. You need to add the constant value and weak link the CoreFoundation framework:
Add this line to your AppDelegate.m:
extern NSString * const NSURLIsExcludedFromBackupKey _attribute_((weak_import));
Add a new value for “Other Linker Flags” in your project’s Build Settings:
-weak_framework CoreFoundation
File them at the Cordova Issue Tracker


To view the demo, please visit the following links:
To download this note, you can print this web page as PDF.
Disclaimer (16 May 2020): I know this page looks like mess. I tried to convert this from a LaTeX document to a HTML webpage (and failed miserably). After studying Engineering for one year, my approach to Oscillation for beginners will be totally different, but it's too much work to rewrite this page.
Meanwhile, I should contemplate a better way to communicate math ideas on GitHub pages.
Simple Harmonic Motion is characterised by the following equation:
$\frac{d^2x}{dt^2} = - \omega ^2 x$
There are some interesting properties of the above equation:
The full solution to this differential equation is:
$x(t) = A \cos(\omega t + \beta)$
$x(t) = A \cos \omega t + B \sin \omega t$
where $A$, $B$ and $\beta$ are real constants.
Total energy of an oscillating system usually exists in two forms: potential energy, a function of position, and kinetic energy, a function of velocity. If we consider a mass-spring system, potential energy and kinetic energy can be expressed as the following:
$V(x) = \frac{1}{2}kx^2 = \frac{1}{2}k A^2 \cos^2 \omega t$
$T(v) = \frac{1}{2}mv^2 = \frac{1}{2}m \omega ^2 A^2 \sin^2 \omega t$
Total energy of the system: $E(x,v) = kA^2$. Energy is conserved, as expected. And this total energy is equal to maximum kinetic energy and maximum potential energy.
NOTE: $m\omega^2 = k$
The oscillating system can be viewed as exchanging potential and kinetic energy periodically, via a force derived from a conservative field. In the case of mass-spring system, kinetic energy is from the moving mass (spring is considered massless, so it doesn't have kineic energy), potential energy is stored in the spring (elastic potential energy) and the force is the spring force.
Any system carrying out small oscillation around an equilibrium position is said to be in SHM. This can be shown by considering an arbitrary one dimensional potential, which is a function of position $V(x)$.
Suppose the function is convex at a particular poitn $x=a$. By evaluating the Taylor series of $V(x)$ at $x=a$ we obtain:
$V(x) = V(a) + \frac{1}{1!} \frac{d}{dx} V(a) . (x-a) + \frac{1}{2!} \frac{d^2}{dx^2} V(a) . (x-a)^2 + ...$
When the oscillation about $x=a$ is small, higher order of $(x-a)^n$ is negligible. Also note that because $\frac{d}{dx}V(a) = 0$, we will have:
$V(x) - V(a) = k(x-a)^2$
$F(x) = -\frac{dV}{dx} = -2k(x-a)$
$\frac{d^2x}{dt^2} = -\frac{2k}{m} (x-a)$
If we choose $(a,0)$ as the new origin, $(x-a)$ will become $x$ while the second time derivative of $x$ stays the same.
$\frac{d^2x}{dt^2} = -\frac{2k}{m} x$
which is the equation of motion for SHM.
NOTE: see Taylor series for a more detailed explanation about the Taylor series.
A mass $m$ is attached to a massless spring with a spring constant $k$. The spring obeys Hooke's Law in both extension and contraction.
To view a demonstration for a simple pendulum system, please visit here.
A point mass $m$ is attached to one end of an massless, inelastic string (or a solid rod) of lenght $L$. The mass is displaced and released from rest from a certain height.
A cylinder of diamter $d$ floats with $l$ of its length submerged. The total height is $L$. The cylinder is pushed down by a distance of $A$ and released.
A vertical tube with a cross-sectional area of $A$ is filled with air of density $\rho$, under adiabatic condition (no heat transfer), is closed at one end and fitted with a freely-moving piston of mass $m$. The piston is pushed down and released.
NOTE: under adiabatic condition, the first law of thermodynamics shows that:
$dU = -PdV$
An LC circuit is composed of an ideal capacitor with capacitance $C$ and an ideal inductor with inductance $L$. The two components are connected to each other (shown below). The capacitor is initially charged to a voltage $V_0$. Find the current in the circuit as a function of time.
Real oscillating systems must dissipate energy and come to a stop. In many situations, the resistive force is proportional to the velocity of the oscillator. We will include a resistive term $F = -\gamma \frac{dx}{dt}$ in the equation of motion.
$\frac{d^2x}{dt^2} = -\omega_0^2x - \gamma\frac{dx}{dt}$
where $\gamma$ is a positive, real constant. It determines the strength the resistive force. $\omega_0$ is the natural frequency, the angular frequency of free oscillation.
Let's again consider some of important features of this ODE:
Although the equation is in real domain ($x(t) \in \mathbb{R}$), it turns out that it's much easier to solve the ODE if we do it in complex domain $\mathbb{C}$.
This particular trick works because a complex function is a linear combination of a real part and an imaginary part. Since time is in the real domain ($t \in \mathbb{R}$), time derivative of a complex function will have a separate real and imaginary parts. To understand this idea, we can write a complex function of time as $z(t)=a(t)+b(t)i$. If we plug this into the above ODE:
$\frac{d^2z}{dt^2} = -\omega_0^2z-\gamma\frac{dz}{dt}$
$\frac{d^2a}{dt^2} + \frac{d^2b}{dt^2}i = -\omega_0^2a -\omega_0^2bi - \gamma\frac{da}{dt} -\gamma\frac{db}{dt}i$
The above equation requires that the real parts equal to the real parts, and the imaginary parts equal to the imaginary parts. Note that the first and second time derivatives of $a(t)$ and $b(t)$ are real functions.
$\frac{d^2a}{dt^2} = -\omega_0^2a-\gamma\frac{da}{dt}$
$\frac{d^2b}{dt^2} = -\omega_0^2b-\gamma\frac{db}{dt}$
This means that both $a(t)$ and $b(t)$ are real solutions to the original ODE i.e. $a(t)$ and $b(t)$ are what we obtain if we solve the ODE in the real domain. Thus, what we can do is that we can solve the damped oscillation ODE in the complex domain, and then obtain the real part of that complex solution to get our real solution.
There are many tricks to solve this ODE, especially in the complex domain. We can try using an exponential function because its derivative has a similar form to itself. So I will let $x(t) = Ae^{Bt}$, where $A$ and $B$ are complex constants. Its first and second time derivatives will be:
$\frac{dx}{dt} = BAe^{Bt}$
$\frac{d^2x}{dt^2} = B^2Ae^{Bt}$
Let's substitute these back into our original ODE and rearrang it:
$B^2Ae^{Bt} = -\omega_0^2Ae^{Bt} - \gamma \frac{dx}{dt} = BAe^{Bt}$
$B^2 = -\omega_0^2 - \gamma B$
$B^2 + \gamma B + \omega_0^2 = 0$
This is our familiar quadratic equation. Because $B$ is a complex number, we can always find the value of B from the above equation. Surprisingly, it also means that the value of $B$ depends entirely on characteristic of our damped oscillation system ($\omega_0$ and $\gamma$). Let's consider our discriminant $\Delta = \gamma^2 - 4\omega_0^2$
$B = -\gamma/2 = -\omega_0$
Our $B$ value is a real number! Our $A$ value will be one adjustable constant for our general solution.
$x(t) = Ae^{-\frac{\gamma}{2}t}$
This is great! As $A$ is our adjustable constant, we can get a real solution by choosing a real value for $A$.
You might note that we still need one more adjustable constant to obtain the general solution. Thus, we need another solution to the ODE. This solution is not intuitive to guess, but it is $x(t) = Ate^{Bt}$. Its first and second time derivatives will be:
$\frac{dx}{dt} = Ae^{Bt} + BAte^{Bt} = (1+Bt)Ae^{Bt}$
$\frac{d^2x}{dt^2} = BAe^{Bt} + (1+Bt)BAe^{Bt} = (2+Bt)BAe^{Bt}$
Substituting these back into our ODE:
$(2+Bt)BAe^{Bt} = -\omega_0^2 Ate^{Bt} - \gamma (1+Bt)Ae^{Bt}$
$(2+Bt)B = -\omega_0^2 t - \gamma (1+Bt)$
$2B+B^2t = -\omega_0^2 t - \gamma - \gamma B t$
$(B^2 + \gamma B + \omega_0^2)t + (2B + \gamma) = 0$
This looks interesting! There is a small observation we can make about this. The left-hand side of the above equation can be thought as a function of time. This function is always equal to zero, which means that all of its coefficients are zero.
$B^2 + \gamma B + \omega_0^2 = 0$
$2B + \gamma = 0$
What a coincidence! This will give us the exact value of $B$ as the above case: $B = -\gamma/2$. Thus our second solution will $x(t) = Ate^{-\frac{\gamma}{2}t}$.
The general solution will be the linear combination of two solutions above:
$x(t) = (A_1+A_2t)e^{-\frac{\gamma}{2}t}$
This situation is also known as Critical damping. The system decays exponentially without oscillation. The amount of damping is just right to stop oscillation.
$B = -\frac{-\gamma \pm \sqrt{\Delta}}{2} = -\frac{\gamma}{2} \pm \sqrt{\frac{\gamma^2}{4}-\omega_0^2}$
Great! We have two values of $B$, which correspond to two solutions:
$x(t) = Ae^{(-\gamma/2 + \sqrt{\gamma^2/4-\omega_0^2})t}$
$x(t) = Ae^{(-\gamma/2 - \sqrt{\gamma^2/4-\omega_0^2})t}$
The general solution will be the linear combination of the above two solutions:
$x(t) = e^{-\frac{\gamma}{2} t} \bigg(A_1e^{\sqrt{\gamma^2/4-\omega_0^2}t}+A_2e^{-\sqrt{\gamma^2/4-\omega_0^2}t}\bigg)$
Again, we can choose the values of $A_1$ and $A_2$ to be real to obtain the real solution.
This situation is known as overdamping. The system decays slowlier than exponentially. The amount of damping is so great that it takes longer for the system to return to the equilibrium position.
$B = -\frac{-\gamma \pm i\sqrt{-\Delta}}{2} = -\frac{\gamma}{2} \pm i\sqrt{\omega_0^2-\frac{\gamma^2}{4}}$
Again, each value of $B$ corresponds to one solution:
$x(t) = Ae^{(-\gamma/2 + i\sqrt{\omega_0^2-\gamma^2/4})t}$
$x(t) = Ae^{(-\gamma/2 - i\sqrt{\omega_0^2-\gamma^2/4})t}$
However, it must be noted that our values of $B$ are complex numbers, and unfortunately, we cannot ignore this fact. We have to take the real part of the above solutions. Luckily, the Euler identity allows us to write the above solutions in a clearer form, to see the real and imaginary parts.
$x(t) = Ae^{-\frac{\gamma}{2} t} \Bigg[\cos\bigg(\sqrt{\omega_0^2-\frac{\gamma^2}{4}}t\bigg) + i\sin\bigg(\sqrt{\omega_0^2-\frac{\gamma^2}{4}}t\bigg)\Bigg]$
$x(t) = Ae^{-\frac{\gamma}{2} t} \Bigg[\cos\bigg(\sqrt{\omega_0^2-\frac{\gamma^2}{4}}t\bigg) - i\sin\bigg(\sqrt{\omega_0^2-\frac{\gamma^2}{4}}t\bigg)\Bigg]$
The real part of the solution above will give us a real solution. Howver, both above solutions have the same real part, thus we will not get two distinct solutions by taking the real part of the two solutions. This is indeed very unfortunate. But interestingly, the imaginary part of the complex solution is also a real solution.
Taking the imaginary part alone (without the imaginary unit $i$) will give us another real solution. Therefore, our two real distinct solutions are:
$x(t) = Ae^{-\frac{\gamma}{2} t} \cos\bigg(\sqrt{\omega_0^2-\frac{\gamma^2}{4}}t\bigg)$
$x(t) = Ae^{-\frac{\gamma}{2} t} \sin\bigg(\sqrt{\omega_0^2-\frac{\gamma^2}{4}}t\bigg)$
The general solution will be a linear combination of the above solutions:
$x(t) = e^{-\frac{\gamma}{2} t} \Bigg[A_1 \cos\bigg(\sqrt{\omega_0^2-\frac{\gamma^2}{4}}t\bigg) + A_2 \sin\bigg(\sqrt{\omega_0^2-\frac{\gamma^2}{4}}t\bigg)\Bigg]$
The general solution shows that this is an oscillating system from the term $\cos$ and $\sin$. Thus, the quantity $\sqrt{\omega_0^2-\frac{\gamma^2}{4}}$ is the angular frequency of oscillation. With this information, we can then set $\omega = \sqrt{\omega_0^2-\frac{\gamma^2}{4}}$ and simplify our general solution:
$x(t) = e^{-\frac{\gamma}{2} t} \bigg(A_1 \cos \omega t + A_2 \sin \omega t \bigg)$
We can make an interesting observation here. Using the Cauchy–Schwarz inequality, we get this:
$A_1 \cos \omega t + A_2 \sin \omega t \leq \sqrt{A_1^2+A_2^2} \sqrt{\cos^2 \omega t + \sin^2 \omega t} = \sqrt{A_1^2+A_2^2}$
Note that $\cos^2{\theta} + \sin^2{\theta} = 1$ for all real values of $\theta$. Thus:
$x(t) \leq \sqrt{A_1^2+A_2^2} e^{-\frac{\gamma}{2}}$
The above inequality means that our general solution is always smaller than an exponential function. This exponential function $\sqrt{A_1^2+A_2^2} e^{-\frac{\gamma}{2}}$ is known as the envelope of our solution: the system will oscillate within this exponential decay envelope.
This is the most interesting situation, also known as underdamping. The amplitude of oscillation decays exponentially with time until there is no more oscillation. The system oscillates at an angular frequency slightly below its natural frequency. The amount of damping is small, dissipating the energy of oscillation.
Note that our general solution can be written in a more compact form:
$x(t) = Ae^{-\frac{\gamma}{2} t}\cos (\omega t+\phi)$
At this point, it's best to visit the Harmonic Oscillator solution graph to understand the behavior of the system when the value of $\gamma$ changes. Keep in mind that you should set the value of $F_0$ to zero.
All of the situations above do not involve an external driving force. Suppose we want to use a force to drive the oscillator. There are many forms that our driving force can take, but for simplicity, we will take the driving force to be of the form $F(t)=F_0 \cos \omega_d t$, where $\omega_d$ is the angular frequency of the driving force. This force is an oscillating force, a worthy assumption for our oscillating system. The ODE then becomes:
$\frac{d^2x}{dt^2}=-\omega_0^2x+\frac{F_0}{m}\cos \omega_d t$
Let's make some observations about this ODE:
This fact will be an obstacle for us, but there is a little trick to circumvent this. I will discuss it later.
Although this ODE is in the real domain, again, it's much easier to analyse and solve it in the complex domain. Remember, our real solution is the real part of our complex solution. Thus, instead of considering our driving force as $F(t) = F_0 \cos \omega_d t$, we will consider our driving force as a complex exponential function of time $F(t) = F_0 e^{i\omega_d t}$. We can do this thanks to the Euler identity. Our ODE in the complex domain will be:
$\frac{d^2x}{dt^2}=-\omega_0^2x+\frac{F_0}{m}e^{i\omega_d t}$$
We will guess our solution to be an exponential function again. However, as you might have observed, we have the driving force term, which has its own exponential term. Thus, we can try an exponential function with the same power as the driving force term as our solution. In the Physics sense, we can understand that our oscillating system follows the angular frequency of the driving force.
$$x=Ae^{i \omega_d t}$$ $$\frac{dx}{dt}=i\omega_dAe^{i \omega_d t}$$ $$\frac{d^2x}{dt^2}=-\omega_d^2Ae^{i \omega_d t}$$Substituting these into our ODE:
$$-\omega_d^2Ae^{i \omega_d t}=-\omega_0^2Ae^{i \omega_d t}+\frac{F_0}{m}e^{i\omega_d t}$$ $$-\omega_d^2A=-\omega_0^2A+\frac{F_0}{m}$$ $$(\omega_0^2-\omega_d^2)A=\frac{F_0}{m}$$ $$A = \frac{F_0/m}{\omega_0^2-\omega_d^2}$$This is indeed very strange! Remember from the above situations, the $A$ value will be one of our adjustable constants. But in this case, we get an exact and real value of $A$! Although we are happy that the complex solution $x(t)=Ae^{i\omega_d t}$ works, this is a fixed solution: we cannot modify this solution to fit to our initial conditions.
At least we know that the corresponding real solution will simply be:
$$x(t) = A\cos \omega_d t$$where $A = \frac{F_0/m}{\omega_0^2-\omega_d^2}$.
This particular solution has a special name: the steady-state solution. This solution is the dominant behavior of the oscillating system after a long period time, when the initial conditions no longer matter much. To fully understand this concept, please continue reading.
We will use a clever trick here. Note that our ODE has an extra driving force term. This term prevents us from adding two solutions together to obtain another solution. However, if we add a solution of free oscillation ODE to a solution of driven oscillation ODE, the newly obtained solution will not affect the driving force term. To see this more clearly, consider $x_1(t)$ as a solution to free oscillation ODE and $x_2(t)$ as a solution to driven oscillation ODE:
$$\frac{d^2x_1}{dt^2} = -\omega_0^2 x_1$$ $$\frac{d^2x_2}{dt^2} = -\omega_0^2 x_2 + \frac{F_0}{m}\cos \omega_d t$$ $$\frac{d^2(x_1+x_2)}{dt^2} = -\omega_0^2 (x_1+x_2) + \frac{F_0}{m}\cos \omega_d t$$Wow! $x_1(t)+x_2(t)$ is a solution to the driven oscillation ODE! Recall the solution to the free oscillation ODE is $x_1(t)=A\cos(\omega t+\phi)$, our general solution to the driven oscillation ODE is:
$$x(t) = A\cos(\omega t+\phi) + \frac{F_0/m}{\omega_0^2-\omega_d^2}\cos \omega_d t$$where $A$ and $\phi$ are our two adjustable constants.
However there is a problem to this solution. This is a sum of two cosine terms with different angular frequencies, which will produce a beat pattern. Visit Harmonic Oscillator solution graph and set $\gamma$ to zero to observe this phenomenon.
Taking a closer look at our steady state solution:
$$x(t) = \frac{F_0/m}{\omega_0^2-\omega_d^2}\cos \omega_d t$$The amplitude of this oscillation depends on the magnitude of the driving force $F_0$, the angular frequency of the driving force $\omega_d$ and the natural frequency of the oscillating system $\omega_0$.


- CloneType - Enum in cz.muni.fi.virtualtoolmanager.pubapi.types
-
Enumeration class that is used for determining what type of virtual machine
clone should be created.
- cloneVirtualMachine(VirtualMachine, CloneType) - Method in class cz.muni.fi.virtualtoolmanager.logicimpl.VirtualizationToolManagerImpl
-
- cloneVirtualMachine(VirtualMachine, CloneType) - Method in interface cz.muni.fi.virtualtoolmanager.pubapi.managers.VirtualizationToolManager
-
Method that creates the virtual machine clone from the given virtual
machine and according to specified clone type.
- close() - Method in class cz.muni.fi.virtualtoolmanager.logicimpl.ConnectionManagerImpl
-
- close() - Method in class cz.muni.fi.virtualtoolmanager.logicimpl.VirtualizationToolManagerImpl
-
- close() - Method in interface cz.muni.fi.virtualtoolmanager.pubapi.managers.ConnectionManager
-
Method that ensures the termination of the code, respectively after this method
call are all connected physical machines disconnected and no virtual
machine operation can be performed.
- close() - Method in interface cz.muni.fi.virtualtoolmanager.pubapi.managers.VirtualizationToolManager
-
Method that ensures all running virtual machines on a particular physical
machine are shut down.
- ClosingActionType - Enum in cz.muni.fi.virtualtoolmanager.pubapi.types
-
Enumeration class that is used for determining what final actions should be
performed before the physical machine is disconnected.
- compareTo(PhysicalMachine) - Method in class cz.muni.fi.virtualtoolmanager.pubapi.entities.PhysicalMachine
-
Method used to compare two physical machines - this with another - in
order to sort (order) physical machines.
- compareTo(PortRule) - Method in class cz.muni.fi.virtualtoolmanager.pubapi.entities.PortRule
-
Method used to compare two port rules - this with another - in
order to sort (order) port rules.
- compareTo(VirtualMachine) - Method in class cz.muni.fi.virtualtoolmanager.pubapi.entities.VirtualMachine
-
Method used to compare two virtual machines - this with another - in
order to sort (order) virtual machines.
- ConnectionFailureException - Exception in cz.muni.fi.virtualtoolmanager.pubapi.exceptions
-
- ConnectionFailureException() - Constructor for exception cz.muni.fi.virtualtoolmanager.pubapi.exceptions.ConnectionFailureException
-
- ConnectionFailureException(String) - Constructor for exception cz.muni.fi.virtualtoolmanager.pubapi.exceptions.ConnectionFailureException
-
- ConnectionFailureException(Throwable) - Constructor for exception cz.muni.fi.virtualtoolmanager.pubapi.exceptions.ConnectionFailureException
-
- ConnectionFailureException(String, Throwable) - Constructor for exception cz.muni.fi.virtualtoolmanager.pubapi.exceptions.ConnectionFailureException
-
- ConnectionManager - Interface in cz.muni.fi.virtualtoolmanager.pubapi.managers
-
Interface that declare what method the implementation of the connection manager
should provide.
- ConnectionManagerImpl - Class in cz.muni.fi.virtualtoolmanager.logicimpl
-
- ConnectionManagerImpl() - Constructor for class cz.muni.fi.virtualtoolmanager.logicimpl.ConnectionManagerImpl
-
- connectTo(PhysicalMachine) - Method in class cz.muni.fi.virtualtoolmanager.logicimpl.ConnectionManagerImpl
-
- connectTo(PhysicalMachine, long) - Method in class cz.muni.fi.virtualtoolmanager.logicimpl.ConnectionManagerImpl
-
- connectTo(PhysicalMachine) - Method in interface cz.muni.fi.virtualtoolmanager.pubapi.managers.ConnectionManager
-
Method that ensures the connection establishment with the required physical
machine on which is present the VirtualBox installation with the web
server that must be running at the moment when there is made an attempt to
establish the connection with the physical machine.
- connectTo(PhysicalMachine, long) - Method in interface cz.muni.fi.virtualtoolmanager.pubapi.managers.ConnectionManager
-
Method that is same as
ConnectionManager.connectTo(PhysicalMachine)
, but with this
method is possible to define the time in milliseconds which determine the
waiting time between each unsuccessful connection establishment attempt.
- countOfCPU(Long) - Method in class cz.muni.fi.virtualtoolmanager.pubapi.entities.SearchCriteria.Builder
-
Sets the number of used virtual CPUs as a search criterion which will be used
during virtual machine search operation.
- countOfCPU(Long) - Method in class cz.muni.fi.virtualtoolmanager.pubapi.entities.VirtualMachine.Builder
-
Sets the number of virtual CPUs which will be used for virtual machine
initialization.
- countOfMonitors(Long) - Method in class cz.muni.fi.virtualtoolmanager.pubapi.entities.SearchCriteria.Builder
-
Sets the number of used monitors as a search criterion which will be used
during virtual machine search operation.
- countOfMonitors(Long) - Method in class cz.muni.fi.virtualtoolmanager.pubapi.entities.VirtualMachine.Builder
-
Sets the number of monitors which will be used for virtual machine
initialization.
- cpuExecutionCap(Long) - Method in class cz.muni.fi.virtualtoolmanager.pubapi.entities.SearchCriteria.Builder
-
Sets the CPU execution limitation as a search criterion which will be used
during virtual machine search operation.
- cpuExecutionCap(Long) - Method in class cz.muni.fi.virtualtoolmanager.pubapi.entities.VirtualMachine.Builder
-
Sets the virtual CPU execution limitation which will by used for the
virtual machine initialization.
- cz.muni.fi.virtualtoolmanager.logicimpl - package cz.muni.fi.virtualtoolmanager.logicimpl
-
- cz.muni.fi.virtualtoolmanager.pubapi.entities - package cz.muni.fi.virtualtoolmanager.pubapi.entities
-
- cz.muni.fi.virtualtoolmanager.pubapi.exceptions - package cz.muni.fi.virtualtoolmanager.pubapi.exceptions
-
- cz.muni.fi.virtualtoolmanager.pubapi.io - package cz.muni.fi.virtualtoolmanager.pubapi.io
-
- cz.muni.fi.virtualtoolmanager.pubapi.managers - package cz.muni.fi.virtualtoolmanager.pubapi.managers
-
- cz.muni.fi.virtualtoolmanager.pubapi.types - package cz.muni.fi.virtualtoolmanager.pubapi.types
-


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Our company will provide our customers with the best value for their money depending on the graphics card that they are purchasing, we will do our utmost best to do price-checking against other companies so that we can best them at prices while we still provide quality reassurance.
Unsatisfied/faulty product.
Don't worry if you are not satisfied on our product/s or if it gets damaged on the way to you, we will allow you to return the product/s and if we cannot get it fixed and personally delivered to you within a work week, we will ensure that you will get your money back guaranteed!
Pricing
Here are some of the refurbished Graphics Cards that we will be selling
ASUS ROG Strix GTX 1060 6GB
$215
- Base & Boost Frequency -> 1506MHz & 1873MHz
- Power Supply Recommended -> 500W
- Memory Size and Type -> 6GB GDDR5/X
- Memory Interface -> 192-bit
- Connectivity -> Displayport 1.4, HDMI 2.0b, USB Type-C & DVI-DL (MAX 8K Resolution @ 60fps)
Gigabyte GeForce RTX 2060
$350
- Base & Boost Frequency -> 1365MHz & 1830MHz
- Power Supply Recommended -> 500W
- Memory Size and Type -> 6GB GDDR6
- Memory Interface -> 192-bit
- Connectivity -> Displayport 1.4 HDR, HDMI, USB Type-C & DVI-DL (MAX 8K Resolution)
MSI AMD Radeon™ RX 580
$160
- Base & Boost Frequency -> 1257MHz & 1393MHz
- Power Supply Recommended -> 500W
- Memory Size and Type -> 8GB GDDR5
- Memory Interface -> 256-bit
- Connectivity -> Displayport 1.4 HDR & HDMI (4K60 Supported)
XFX AMD Radeon™ RX 5600 XT
$320
- Base & Boost Frequency -> 1375MHz & 1560MHz
- Power Supply Recommended -> 550W
- Memory Size and Type -> 6GB GDDR6
- Memory Interface -> 192-bit
- Connectivity -> Displayport 1.4 & HDMI (4K60 Supported)
If you would like to know here we source our parts from, here is a few links to the products listed above if you would like to check it out, these produts are a bit more pricey that is shown on the website, but we will mark it down to the best of our ability so that us and the customer is satisfied:
- XFX Radeon™ RX 5600 XT @ Wootware
- Gigabyte RTX 2060 6GB @ Wootware
- MSI Radeon™ RX 580 8GB Gaming X @ Newegg
- ASUS GeForce GTX 1060 6GB @ Newegg


{% include head.html %}
{% include navigation.html %}Nowadays, People especially introvert millenials, are hardly stepping out of door actively to involve socialization. They really want to make friends with others, but there is NO low-cost or just natural way to know someone new. It's not surprising but interesting social psychology phenomenon and which leads to much more social anxienty and causes self-recognition problems later. Apart from those mainstream social media product across various platfroms like FB, Instagram, Snapchat, Tinder and etc. They have a whole lot of viable social features to have people interact so much, but just don't see a similar channel seamlessly integrated back to real life.
The short-term goal here is to enable location-based social onnections based on home-made food sharing events. The long-term goal here is to resolve monetization strategy (platform ads, feature-based freemium model, partnership with local grocery market and etc) to make this product profitable and sustainable. Figuring out the proper medium is key. It could be achieved via sharing food. So food could become the medium and gather people together naturally. This app is aiming to make socialize connection with local community and nearby neighbours. Why is it? It could be expanded to more target users (Initially will be all Millenials who desire to make friends) after small geographical range of trials on most potential users.
This was completed by Sketch prototype tool.(Great to learn it!)
A little rough but decide to choose mobile platform layout and light warm coloring themes. There are total 9 pages at this point that are involving user interaction. (Seriously thinking of security verification process as this is a wide open app could be used not for being good.) So It could be 10 ~ 12 pages.
Something needs to be re-considered and also re-assess the growth risk.
The goal here is to estimate the buiness star based on the attributes provided in the raw data(will be "business.json") and also give a relatively accurate semantic results on consumer's review.(will be "review.json")
The data input that is originally from Yelp Academic Dataset. With the help of its users, It provides a ealth of information about franchise and vendors. It includes 1,569,264 reviews, spanning from May 2005 to Jan 2015. These reviews are made on 61,184 business records.
Each review contains a one to five stars rating, which indicates customer satisfaction level.
Also the attrivute called "Price Range" is an important player.  Likewise you pay less than 10 bucks and you get medium service then you might think it's ok exprience. So we would like to drop the data entry if it misses this attribute.
Challenges
Logistic regression
K-nearest Neighbors
Confusion Matrix
# import library
from pandas import *
# generate x: is the array of attributes
# generate correlation table and print graph
df = DataFrame(data=x, columns=['longitude','latitude','review_count','Price Range','Noise Level','Accepts Credit Cards','Take-out','Delivery','Wheelchair Accessible','Takes Reservations'])
print df.columns.values.tolist()
cor_matrix = np.corrcoef(df.T)
sm.graphics.plot_corr(cor_matrix,xnames=df.columns.values.tolist())
plt.savefig("f”)
Takeaways
we are able to improve the accuracy from around 45% ~ 50% at the beginning up to around 97% at least. Particularly while dividing target rating range into two categories, Naive bayes, KNN and SVM gave relatively better results other than decision tree.
By limiting 10,000 records from "review.json"(due to CPU performance concern) as also operate analysis the score of every single review record item. If the score is positive, we consider the target star is equal or above 3; if negative, we consider it is less than 3 (Star rating range: 0 ~ 5). The result confidence is 80.31%
Enterprises software and technological buiness are encounting the most sereve security threats from various defects and flaws from their applications. This has been likely much underestimated widely in the whole industry as you can see a bunch of well-known companies became the victim of hundreds lines of flawed codes.
There is no perfect software design and bullet-proof fortification. But we'd better start working on minimum amount of defective data, track them, monitor them and fix them with help of security experts
2 viewpoints(Horizontal view needed) with detailed stats. So users will have a clear grasp on what's going on there with their codebase, checking progress after consulting experts to fix security problems.


aXMLRPC is a Java library with a leightweight XML-RPC client. XML-RPC is a specification for making remote procedure calls over the HTTP protocol in an XML format. The specificationc an be found under http://www.xmlrpc.com/spec.
The library was developed for the use with Android. Since it has no dependencies to any Android library or any other 3rd-party library, it is fully functional in any common java virtual machine (not only on Android).
You can control the client with some flags to extend its functionality. See the section about flags.
How to include the aXMLRPC client into your project? There are three different ways to do that:
You can just include all the source code from the src
directory into the sourcecode
of your project. If you use git yourself, you can use submodules to include the code
as a module to yours. So you will always stay up to date with the library.
The library itself is a NetBeans project and can be compiled either with NetBeans or
with ant
. The resulting JAR file can be used as a dependency in your project. If you
use NetBeans you can make a dependency directly to the project.
You can download a compiled jar file from the above Download tag and use it as a library for your project. This is not recommended, because you will not stay up to date to the sourcecode.
You can use the library by initiating an XMLRPCClient
and make calls over it:
try {
XMLRPCClient client = new XMLRPCClient(new URL("http://example.com/xmlrpc"));
Boolean b = (Boolean)client.call("isServerOk");
Integer i = (Integer)client.call("add", 5, 10);
} catch(XMLRPCServerException ex) {
// The server throw an error.
} catch(XMLRPCException ex) {
// An error occured in the client.
} catch(Exception ex) {
// Any other exception
}
Instead of passing the parameters as seperated values, you can also pack them in an array and pass the array to the method, like in the following example:
// ... The try-catch has been ommited for clarity.
XMLRPCClient client = new XMLRPCClient(url, "MyUserAgentString");
client.call("someMethod", new Object[]{ o1, o2, o3 });
// ...
The above method calls are synchronous. So the method call
will return when the server responded
or an error occured. There is also a possibility for asynchronous server calls.
You need to implement an XMLRPCCallback that will get noticed about the respone (or error) from
the server. The callAsync
method can be used to make asynchronous calls. It returns an identifier
that will also be send to the XMLRPCCallback instance with the response of the server, so your
application can make multiple calls concurrently and use one listener for them, that distinguish
between the different request by their ids.
XMLRPCCallback listener = new XMLRPCCallback() {
public void onResponse(long id, Object result) {
// Handling the servers response
}
public void onError(long id, XMLRPCException error) {
// Handling any error in the library
}
public void onServerError(long id, XMLRPCServerException error) {
// Handling an error response from the server
}
};
XMLRPCClient client = new XMLRPCClient(url);
long id = client.callAsync(listener, "add", 5, 10);
The specification give some data tags for the server response. If you want to work on the
type you must cast the returning Object
from the call
method to its specific type.
Which type to cast which XML server response, tells the following list:
i4
,int
=> Integer
boolean
=> Boolean
string
=> String
double
=> Double
dateTime.iso8601
=> Date
base64
=> byte[]
(Byte[]
won't work)
array
=> Object[]
struct
=> Map<String,Object>
i8
=> Long
(see Flags)
The client takes as second parameter (or third if an user agent is given) a combination of multiple flags. It could work like the following example:
// ...
XMLRPCClient client = new XMLRPCClient(url,
XMLRPCClient.FLAGS_STRICT | XMLRPCClient.FLAGS_8BYTE_INT);
// ...
The following flags are implemented:
The client should parse responses strict to specification. It will check if the given content-type is right. The method name in a call must only contain of A-Z, a-z, 0-9, _, ., :, / Normally this is not needed.
The client will be able to handle 8 byte integer values (longs).
The xml type tag <i8>
will be used. This is not in the specification
but some libraries and servers support this behaviour.
If this isn't enabled you cannot recieve 8 byte integers and if you try to
send a long, the value must be within the 4 byte integer range.
With this flag, the client will be able to handle cookies, meaning saving cookies from the server and sending it with every other request again. This is needed for some XML-RPC interfaces that support login.
The client will be able to send null
values. A null
value will be send
as <nil/>
. This extension is described under: http://ontosys.com/xml-rpc/extensions.php
With this flag enabled, the XML-RPC client will ignore the HTTP status code of the response from the server. According to specification the status code must be 200. This flag is only needed for the use with not standard compliant servers.
With this flag enabled, the client will forward the request, if the 301 or 302 HTTP status code has been received. If this flag is not set, the client will throw an exception on these HTTP status codes.
With this flag enabled, the client will ignore, if the URL doesn't match the SSL Certificate. This should be used with caution. Normally the URL should always match the URL in the SSL certificate, even with self signed certificates.
With this flag enabled, the client will ignore all unverified SSL/TLS certificates. This must be used, if you use self-signed certificates or certificated from unknown (or untrusted) authorities.
The library is licensed under [MIT License] (http://www.opensource.org/licenses/mit-license.php). See the LICENSE file for the license text.
For the uninformed reader: What does MIT mean?
If you find a bug or wish some enhancements for the library, please fill an issue here on github or contact me otherwise (www.timroes.de).


BUT I'M A CHEERLEADER (Lions Gate) Starring: Natasha Lyonne, Clea DuVall, Cathy Moriarty, But Cort, Mink Stole, RuPaul Charles. Screenplay: Brian Wayne Peterson. Producers: Andrea Sperling and Leanna Creel. Director: Jamie Babbit. MPAA Rating: R (profanity, adult themes) Running Time: 85 minutes. Reviewed by Scott Renshaw.
There's something terribly depressing about a wonderful concept turned into mush by someone who doesn't know how to handle it. The irritations of a film like THE REPLACEMENTS are far more mundane by comparison-you know that it will be at best a tolerable audience-friendly mediocrity, at worst a bland, pressed and processed Entertainment McNugget. BUT I'M A CHEERLEADER, on the other hand, could have been a brilliant bit of satire. It could have been the kind of film that, even while preaching to the choir, highlights the magnificent absurdities of a very hot-button issue. It could have been the CITIZEN RUTH of the "gay conversion" movement.
Could've been, but isn't. Jamie Babbit's sloppy, smirking story introduces us to Megan (Natasha Lyonne), a middle-class girl with a boyfriend, good Christian parents (But Cort and Mink Stole) and the enviable life of a high school cheerleader. Her friends and family also believe that she has a secret-namely, that she harbors unnatural, unhealthy desires for other women.  Soon Megan is deep into the five-step program, but she also finds herself interested in a surly fellow "patient" named Graham (Clea DuVall) -- interested in an unnatural, unhealthy desire sort of way.
Somewhere, buried deep in BUT I'M A CHEERLEADER, is the germ of a risky comic idea: that Megan really isn't gay until she comes to True Directions, which in effect converts her contrary to their goals by exposing her to other lesbians. There's something in that idea to anger virtually anyone, only Babbit doesn't pursue it. Instead, she makes it clear from the opening minutes that Megan is repressing latent desires, and that her denials merely represent a state of denial. Even the good gags Babbit wrings from this variation -- like the photo in Megan's school locker -- are underlined too obviously, and never reach into truly daring areas. The campy tone set in the first half-hour, including Moriarty's drag diva performance, show that Babbit isn't particularly interested in scathing humor. Simple mockery suits her just fine.
Even that tone, however, proves to be one she can't sustain. BUT I'M A CHEERLEADER might never have been riotously funny as the silly spoof it initially appears to be, but at least it might have felt consistent. Babbit makes the ridiculous decision to bounce back and forth between scoring points off swishy stereotypes, exploring the conflicts of family reaction to homosexuality and developing an actual romantic sub-plot. There's not nearly enough substance to BUT I'M A CHEERLEADER for its serious side to feel anything but token, and too many misguided serious moments to give it a real comic kick.  And you can feel that potential being crushed under Babbit's leaden heel every time Megan and Graham share a tender moment.
There are plenty of people who take the idea of converting gays and lesbians to heterosexuality very seriously, and plenty of people with same-sex attractions who desperately want such programs to work. Babbit never seems to clue into that fact, or she would base her satire more squarely in the growing popularity of these programs. Instead, she lays out BUT I'M A CHEERLEADER as though the whole idea were self-evidently ludicrous, and gets lazy about finding the humor in people scrambling for conformity, acceptance and easy answers to a challenging issue.  There's no excuse for a subject this incendiary to be the stuff of pratfalls and sappy endings.
On the Renshaw scale of 0 to 10 cheer miseries: 3.
Visit Scott Renshaw's Screening Room http://www.inconnect.com/~renshaw/ *** Subscribe to receive new reviews directly by email! See the Screening Room for details, or reply to this message with subject "Subscribe".
The review above was posted to the
rec.arts.movies.reviews newsgroup (de.rec.film.kritiken for German reviews).
The Internet Movie Database accepts no responsibility for the contents of the
review and has no editorial control. Unless stated otherwise, the copyright
belongs to the author.
Please direct comments/criticisms of the review to relevant newsgroups.
Broken URLs inthe reviews are the responsibility of the author.
The formatting of the review is likely to differ from the original due
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Related links: index of all rec.arts.movies.reviews reviews


|
TouchGFX
v4.13.0
|
A click event. More...
#include <touchgfx/events/ClickEvent.hpp>
Public Types | |
| enum | ClickEventType { PRESSED, RELEASED, CANCEL } |
| The click event types. More... | |
| Public Types inherited from Event | |
| enum | EventType { EVENT_CLICK, EVENT_DRAG, EVENT_GESTURE } |
| The events types. More... | |
Public Member Functions | |
| ClickEvent (ClickEventType type, int16_t x, int16_t y, int16_t force=0) | |
| Constructor. More... | |
| virtual | ~ClickEvent () |
| Destructor. More... | |
| int16_t | getX () const |
| Gets the x coordinate of this event. More... | |
| int16_t | getY () const |
| Gets the y coordinate of this event. More... | |
| void | setX (int16_t x) |
| Sets the x coordinate of this event. More... | |
| void | setY (int16_t y) |
| Sets the y coordinate of this event. More... | |
| void | setType (ClickEventType type) |
| Sets the click type of this event. More... | |
| ClickEventType | getType () const |
| Gets the click type of this event. More... | |
| int16_t | getForce () const |
| Gets the force of the click. More... | |
| virtual Event::EventType | getEventType () |
| Gets event type. More... | |
| Public Member Functions inherited from Event | |
| virtual | ~Event () |
| Destructor. More... | |


About Me
I am a web developer and composer. I am currently in the Web Development Immersive program at General Assembly. When the program finishes I hope to work on server side JavaScript. On the client side I enjoy working in Angular and dabbling in Famo.us(this site for instance)


Akan is a Ghanian tribe
The Akan people of Ghana frequently name their children after the day of the week they were born and the order in which they were born.
These "day names" have further meanings concerning the soul of the person and character.


Stocker
Gainers and Losers
(current)
Mutual fund calculator
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Share Thought
Back-end for a social netwoork that allows users to create thoughts, react to thoughts and add other users as friends.
API Routes
- /api/users to get all users or post a user
- /api/users/userId to get a one user by ID, update a user or delete a user
- /api/users/:userId/friends/:friendId to add or delete a friend
- /api/thoughts to get all thoughts or post a thought
- /api/thoughts/thoughtId to get one thought by ID or update a thought
- /api/thoughts/:userId/:thoughtId to delete a thought
- /api/thoughts/:thoughtId/reactions to add a reaction
- /api/thoughts/:thoughtId/reactions/:reactionId to remove a reaction