Examples of using Mathrm in English and their translations into Italian
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Colloquial
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Official
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Medicine
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Financial
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Ecclesiastic
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Ecclesiastic
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Computer
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Programming
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Official/political
If S t k< 0.1{\displaystyle\mathrm{Stk}<0.1}, tracing accuracy errors are below 1.
The values of$\mathrm{proxmin}$ are stored in the buffer of settings in positions 1 to 7.
t 2.792× 10- 5 s{\displaystyle t=2.792\times 10^{-5}\;\mathrm{s}} which is about 28 microseconds.
W){\displaystyle\mathrm{Hom} V, W.
for S t k≫ 1{\displaystyle\mathrm{Stk}\gg 1}, particles will detach from a flow especially where the flow decelerates abruptly.
It then stores h 999( p a s s w o r d){\displaystyle h^{999}(\mathrm{password})} for the next time the user wishes to authenticate.
For initial tensions between 400{\displaystyle 400} and 600 N{\displaystyle 600\,\mathrm{N}}, there can be slip areas on both sides with a stick area in between.
For example, a server begins by storing h 1000( p a s s w o r d){\displaystyle h^{1000}(\mathrm{password})} which is provided by the user.
In particular, the L-amino acids normally found in proteins can spontaneously isomerize at the C α{\displaystyle\mathrm{C^{\alpha}}} atom to form D-amino acids, which cannot be cleaved by most proteases.
The cancellation of the positive charge on the lysine weakens the electrostatic attraction for the(negatively charged) nucleic acids. sulfation Tyrosines may become sulfated on their O η{\displaystyle\mathrm{O^{\eta}}} atom.
Δ H⊖- 69500 z 2/ r e f f{\displaystyle\Delta H^{\ominus}=-69500\\mathrm{ z^{ 2}/ r_{ eff}}}
If the initial tension is 600 N{\displaystyle 600\,\mathrm{N}} and the tension is reduced to 400 N{\displaystyle 400\,\mathrm{N}}
The effective nuclear charge(often symbolized as Z e f f{\displaystyle Z_{\mathrm{eff}}} or Z∗{\displaystyle Z^{\ast}})
The radius of the nucleus is roughly: R( 1.25× 10- 15 m)× A 1/ 3{\displaystyle R=\left(1.25\times 10^{-15}\mathrm{m}\right)\times A^{1/3}}
T k{\displaystyle\mathrm{rate}=-\ left({\ frac{ d}{ dt}}\ right)_{ T}= k.
related units of length, the other two being the Compton wavelength of the electron λ e{\displaystyle\lambda_{\mathrm{e}}} and the classical electron radius r e{\displaystyle r_{\mathrm{e.
which can be determined from n± ϵ r μ r{\displaystyle\scriptstyle n=\pm{\sqrt{\epsilon_{\mathrm{r}}\mu_{\mathrm{r.
The effective thermal expansion coefficient α e f f{\displaystyle\alpha_{\mathrm{eff}}} is different from the usual thermal expansion coefficient α{\displaystyle\alpha}
Work in units where the gravitational"constant" measured today far from gravitating matter is unity so set G t o d a y α/ c 0 c 1 1{\displaystyle G_{\mathrm{today}}=\alpha/ c_{ 0} c_{ 1} =1.
e. J d r i f t+ J d i f f u s i o n 0{\displaystyle\mathbf{J}_{\mathrm{drift}}+\mathbf{J}_{\mathrm{diffusion}}=0.