CDOT in Turkish translation

• cdot

Examples of using Cdot in English and their translations into Turkish

Hence we arrive at∇⋅ g- 4 π G ρ,{\displaystyle\nabla\cdot\mathbf{g} =-4\pi G\rho,} which is the differential
Hence we arrive at ∇ ⋅ g- 4 π G ρ,{ \displaystyle \nabla \cdot \mathbf{ g}

work per unit time, given by P τ⋅ ω,{\displaystyle P={\boldsymbol{\tau}}\cdot{\boldsymbol{\omega}},} where P is power,
P τ ⋅ ω,{ \displaystyle P={ \boldsymbol{ \tau}} \cdot{ \boldsymbol{ \omega}},} P güç,

P C S W D P C⋅ P H R{\displaystyle P_{CSWD}={\sqrt{P_{C}\cdot P_{HR}}}} The ratio of harmonic means or"Harmonic means" price index is the harmonic average counterpart to the Dutot index.
P C S W D P C ⋅ P H R{ \displaystyle P_{ CSWD}={ \sqrt{ P_{ C} \cdot P_{ HR}}}}'' Harmonik ortalamalar'' fiyat endeksi fiyatlarin t dönemi ile 0 dönemi harmonik ortalaması oranıdır.

In differential form this continuity equation becomes:∇⋅ J f-∂ ρ f∂ t,{\displaystyle\nabla\cdot{\boldsymbol{J_{f\frac{\partial\rho_{f}}{\partial t}}\,} where the left side is the
Diferansiyel formda, bu süreklilik denklemi şu hale gelir: ∇ ⋅ J f- ∂ ρ f ∂ t,{ \displaystyle \nabla{ \boldsymbol{ \cdot J_{ f \frac{ \partial \rho_{ f}}{ \partial t}}\,}

In this sense, the function χ(⋅){\displaystyle\chi(\cdot)} and P i j…(⋅){\displaystyle\ P_{ij\ldots}(\cdot)} are single-valued and continuous,
Bu anlamda χ( ⋅){ \displaystyle \chi( \cdot)} and P i j…( ⋅){ \displaystyle\ P_{ ij\ldots}( \cdot)} fonksiyonları tek değerli ve süreklidirler,

\cdot {\vec {\omega}}dt.}
\mathbf{ T} \cdot{ \vec{ \omega}}

Substituting this in Gauss's law gives∇ 2 Φ M∇⋅ M.{\displaystyle\nabla^{2}\Phi_{M}=\nabla\cdot\mathbf{M}.} Thus, the divergence of the magnetization,∇⋅ M,{\displaystyle\scriptstyle\nabla\cdot\mathbf{M},} has a role analogous to the electric charge in electrostatics and is often referred to as an effective charge density ρ M{\displaystyle\rho_{M.
Bunu Gauss yasasında yerine koyarsak, ∇ 2 Φ M ∇ ⋅ M.{ \displaystyle \nabla^{ 2} \Phi_{ M} =\nabla \cdot \mathbf{ M}.} Bu nedenle mıknatıslanmanın ıraksaması, ∇ ⋅ M,{ \displaystyle \scriptstyle \nabla \cdot \mathbf{ M},} elektrostatikteki elektrik yüklerinin analojisinde bir role sahiptir ve genelde yük yoğunluğu ρ M{ \displaystyle \rho_{ M}} olarak gösterilir.

x)\approx a(t, x)e^{i(k\cdot x-\omega t)}} where k, ω{\displaystyle k,\omega}
e i( k ⋅ x- ω t){ \displaystyle u( t,

Cdot was it? Is this us getting to know each other?
Birbirimizi tanıma çabası mı bunlar? CDOT mıydı?

Geometrically, the scalar triple product a⋅( b× c){\displaystyle\mathbf{a}\cdot(\mathbf{b}\times\mathbf{c})} is the(signed) volume of the parallelepiped
Geometrik olarak, skaler üçlü çarpım a ⋅( b × c){ \displaystyle \mathbf{ a} \cdot( \mathbf{ b}

one has∇⋅ D ρ f{\displaystyle\mathbf{\nabla}\cdot\mathbf{D}=\rho_{f}} where∇⋅{\displaystyle\mathbf{\nabla}\cdot} is the divergence operator,
∇ ⋅{ \displaystyle \mathbf{ \nabla} \cdot}, Diverjansa D{ \displaystyle \mathbf{ D}},

is defined by the line integral φ( r)-∫ C E⋅ d l{\displaystyle\varphi\mathbf{(r)}=-\int_{C}\mathbf{E}\cdot\mathrm{d}\mathbf{l}} where φ(r)
φ E- ∫ C E ⋅ d s,{ \displaystyle \varphi_{ \mathbf{ E}} =-\int_{ C} \mathbf{ E} \cdot \mathrm{ d}

equals a⋅( b× c) ε i j k a i b j c k.{\displaystyle\mathbf{a}\cdot(\mathbf{b\times c})=\varepsilon_{ ijk}
ε i j k a i b j c k.{ \displaystyle \mathbf{ a} \cdot( \mathbf{ b\times c})

as a Stark shift, E S- d⋅ F.{\displaystyle E_{\ text{ S}}=-\ mathbf{d}\cdot\mathbf{F}.} Depending on the sign of the projection of the dipole moment onto the local electric field vector,
E S- d ⋅ F.{ \displaystyle E_{ \text{ S}} =-\mathbf{ d} \cdot \mathbf{ F}.} Yerel elektrik alan vektöründeki bir çiftkutbun yansıma işaretine bağlı olarak bir durum alan sertliğini artıran ya

d W d t P( t) F⋅ v.{\displaystyle{\frac{ dW}{ dt}}= P( t)=\ mathbf{F}\cdot\mathbf{v}.} If the work for an applied force is independent of the path,
F ⋅ v.{ \displaystyle{ \frac{ dW}{ dt}} =P( t) =\mathbf{ F} \cdot \mathbf{ v}.} Eğer uygulanan kuvvet için iş yoldan bağımsız ise,

Thus Abraham also derived the"transverse mass": m T 3 4⋅ m e m⋅ 1 β 2{\displaystyle m_{T}={\frac{3}{4}}\cdot m_{em}\cdot{\frac{1}{\beta^{2}}}\left} On the other hand, already in 1899
Böylece Abraham enine kütle yi de türetti: m T 3 4 ⋅ m e m ⋅ 1 β 2{ \displaystyle m_{ T}={ \frac{ 3}{ 4}} \cdot m_{ em} \cdot{ \frac{ 1}{ \beta^{ 2}}}