OmegaT information

multiplatform CAT tool / Code / [86775c] /Release/OmegaT-license.TXT". "Chapter 1. Installing and running OmegaT". omegat.sourceforge.io. Retrieved 2019-08-14. "Results...

Omega (US: /oʊˈmeɪɡə, -ˈmɛɡə, -ˈmiːɡə/, UK: /ˈoʊmɪɡə/; uppercase Ω, lowercase ω; Ancient Greek ὦ, later ὦ μέγα, Modern Greek ωμέγα) is the twenty-fourth...

com. November 17, 2010. Retrieved October 7, 2017. "OmegaT, the free translation memory tool". Omegat.org. Archived from the original on January 25, 2016...

the localisation process of a software product. Some CAT tools like OmegaT, OmegaT+, Swordfish or Sun's Open language tools can specifically handle resource...

){\mathcal {L}}^{-1}\left\{{\frac {\omega }{s^{2}+\omega ^{2}}}\right\}\\&=\sin(\varphi )\cos(\omega t)+\cos(\varphi )\sin(\omega t).\end{aligned}}} This is just...

\scriptstyle {\widehat {g}}(\omega )} t {\displaystyle \scriptstyle t} ω {\displaystyle \scriptstyle \omega } t {\displaystyle \scriptstyle t} ω {\displaystyle \scriptstyle...

{\begin{aligned}u(x,t)&=\int _{-\infty }^{\infty }s_{+}(\omega )e^{-i(kx+\omega t)}\,d\omega +\int _{-\infty }^{\infty }s_{-}(\omega )e^{i(kx-\omega t)}\,d\omega \\&=\int...

{\displaystyle G(\omega )={\frac {2\zeta \omega _{0}\omega }{\sqrt {\left(2\omega \omega _{0}\zeta \right)^{2}+(\omega _{0}^{2}-\omega ^{2})^{2}}}}.} The...

t + ϕ ) = 1 2 [ e j ( ω t + ϕ ) + e − j ( ω t + ϕ ) ] {\displaystyle \ \cos(\omega t+\phi )={\frac {1}{2}}{\Big [}e^{j(\omega t+\phi )}+e^{-j(\omega t+\phi...

{p}}^{2}}{2m}}+{\frac {1}{2}}m\omega ^{2}{\hat {x}}^{2}\,,} where m is the particle's mass, k is the force constant, ω = k / m {\textstyle \omega ={\sqrt {k/m}}} is...

{(\omega t)},{\frac {\hbar }{2m\Omega }}\left(\cos ^{2}(\omega t)+{\frac {\Omega ^{2}}{\omega ^{2}}}\sin ^{2}{(\omega t)}\right)\right)} | Φ ( p , t )...

(u)(t)={\begin{cases}+u_{m}(t)\cdot \sin(\omega t+\varphi ),&\omega >0,\\-u_{m}(t)\cdot \sin(\omega t+\varphi ),&\omega <0.\end{cases}}} A specific type...

time t is y R ( x , t ) = y max sin ⁡ ( 2 π x λ − ω t ) . {\displaystyle y_{\text{R}}(x,t)=y_{\text{max}}\sin \left({2\pi x \over \lambda }-\omega t\right)...

t ) x ^ + r ω cos ⁡ ( ω t ) y ^ , {\displaystyle {\textbf {v}}={\dot {\textbf {r}}}=-r\omega \sin(\omega t){\hat {\mathbf {x} }}+r\omega \cos(\omega t){\hat...

{\begin{aligned}{\frac {d}{dt}}[A\sin(\omega t+\varphi )]&=A\omega \cos(\omega t+\varphi )\\&=A\omega \sin(\omega t+\varphi +{\tfrac {\pi }{2}})\,.\end{aligned}}} A...

represented as V ( t ) = V 0 e j ω t = V 0 ( cos ⁡ ω t + j sin ⁡ ω t ) , {\displaystyle V(t)=V_{0}e^{j\omega t}=V_{0}\left(\cos \omega t+j\sin \omega t\right),}...

function: x ( t ) = c 1 cos ⁡ ( ω t ) + c 2 sin ⁡ ( ω t ) , {\displaystyle x(t)=c_{1}\cos \left(\omega t\right)+c_{2}\sin \left(\omega t\right),} where...

x_{\text{c}}(t)=x_{i}{\frac {\sin \omega (t_{f}-t)}{\sin \omega (t_{f}-t_{i})}}+x_{f}{\frac {\sin \omega (t-t_{i})}{\sin \omega (t_{f}-t_{i})}}.} This trajectory...

( 1 ) ( ω , T ) = 1 T | ∫ 0 T e i ω t X t d t | 2 , {\displaystyle S^{(1)}(\omega ,T)={\frac {1}{T}}\left|\int _{0}^{T}e^{i\omega t}X_{t}dt\right|^{2}...

{\omega }}_{1}&=-(I_{3}-I_{2})\omega _{3}\omega _{2}~~~~~~~~~~~~~~~~~~~~{\text{(1)}}\\I_{2}{\dot {\omega }}_{2}&=-(I_{1}-I_{3})\omega _{1}\omega...

/2}\omega e^{i\omega t}\right)\\={}&\operatorname {Re} \left(\omega Ae^{i(\theta +\pi /2)}\cdot e^{i\omega t}\right)\\={}&\omega A\cdot \cos \left(\omega...

W 2 = A [ cos ⁡ ( k x − ω t ) + cos ⁡ ( k x − ω t + φ ) ] . {\displaystyle W_{1}+W_{2}=A[\cos(kx-\omega t)+\cos(kx-\omega t+\varphi )].} Using the trigonometric...

{dR}{dt}}\omega {\begin{bmatrix}-\sin(\omega t+\pi /4)\\\cos(\omega t+\pi /4)\end{bmatrix}}-\omega ^{2}R(t){\begin{bmatrix}\cos(\omega t+\pi /4)\\\sin(\omega t+\pi...

dU={\frac {1}{2}}\ dm\omega ^{2}\ y^{2}={\frac {1}{2}}\ \mu dx\omega ^{2}\ A^{2}\sin ^{2}\left({\frac {2\pi x}{\lambda }}-\omega t\right)} And the potential...

{dt}}{{\partial T} \over {\partial {\vec {\omega }}}}&={{\partial T} \over {\partial {\vec {\omega }}}}\times {\vec {\omega }}+{{\partial T} \over {\partial...

ω 1 t ) , {\displaystyle x(t)=e^{-\beta t}\left(C_{1}e^{\omega _{1}t}+C_{2}e^{-\omega _{1}t}\right),} where ω 1 = β 2 − ω 0 2 {\textstyle \omega _{1}={\sqrt...

_{\Omega (t)}i_{\mathbf {v} }(d_{x}\omega )+\int _{\partial \Omega (t)}i_{\mathbf {v} }\omega +\int _{\Omega (t)}{\dot {\omega }},} where Ω(t) is a time-varying...