T_s=T₀ \left[1+r\left(\frac{\gamma -1}{2}\right)M{a}^2\right]

Z_in=η₁ \frac{{\eta }_{\mathrm{m}}+{\eta }_1\tanh \left({\gamma }_1{d}_1\right)}{{\eta }_1+{\eta }_{\mathrm{m}}\tanh \left({\gamma }_1{d}_1\right)}

R= \frac{Z_{\mathrm{in}}-{\eta }_0}{Z_{\mathrm{in}}+{\eta }_0}

R= \frac{Z_{\mathrm{in}}/{\eta }_0-1}{Z_{\mathrm{in}}/{\eta }_0+1} = \frac{{\eta }_1\tanh \left({\gamma }_1{d}_1\right)/{\eta }_0-1}{{\eta }_1\tanh \left({\gamma }_1{d}_1\right)/{\eta }_0+1}

R'=20lg|R|=20lg \left|\frac{{\eta }_1\tanh \left({\gamma }_1{d}_1\right)/{\eta }_0-1}{{\eta }_1\tanh \left({\gamma }_1{d}_1\right)/{\eta }_0+1}\right|

\sqrt[]{\frac{{\mu }_0}{{\epsilon }_0}} =η₁tanh(γ₁ d₁)= \sqrt[]{\frac{{\mu }_0{\mu }_r}{{\epsilon }_0{\epsilon }_r}} tanh(γ₁ d₁)

L(X)=exp \left[{\alpha }_0+\stackrel{n}{\sum _{j=1}}{\alpha }_j{X}_j\right]

L=exp \left[{\alpha }_0+{\alpha }_1\frac{1}{T}+{\alpha }_2\ln I_{\mathrm{UV}}\right] = e^{{\alpha }_0} e^{{\alpha }_1\frac{1}{T}} I_{\mathrm{UV}}^{{\alpha }_2}

lnL=α₀+α₁ \frac{1}{T} +α₂I_UV

f(t)= \frac{\beta }{\eta } {\left(\frac{t}{\eta }\right)}^{\beta -1} exp \left(-{\left(\frac{t}{\eta }\right)}^{\beta }\right)

=βt^β-1 e^{-\beta \left({\alpha }_0+{\alpha }_1\frac{1}{T}+{\alpha }_2\ln I_{\mathrm{UV}}\right)} · e^{-t^{\beta }{e}^{-\beta \left({\alpha }_0+{\alpha }_1\frac{1}{T}+{\alpha }_2\ln I_{\mathrm{UV}}\right)}}

∧=lnf(t)

= \stackrel{F}{\sum _{i=1}} ln \left[\beta T_i^{\beta -1}{e}^{-T_i^{\beta }{e}^{-\beta \left({\alpha }_0+\stackrel{n}{\sum _{j=1}}{\alpha }_j{X}_{i,j}\right)}}{e}^{-\beta \left({\alpha }_0+\stackrel{n}{\sum _{j=1}}{\alpha }_j{X}_{i,j}\right)}\right]

- \stackrel{S}{\sum _{i=1}} (T'_i)^β e^{-\beta \left({\alpha }_0+\stackrel{n}{\sum _{j=1}}{\alpha }_j{X}_{i,j}\right)}

\frac{\partial \wedge }{\partial \beta } =0

\frac{\partial \wedge }{\partial {\alpha }_i} =0,(i=0,…,n)

\stackrel{\text{̅}}{L} =ηΓ \left(\frac{1}{\beta }+1\right)

Γ(x)= {\int }_0^{\infty } e^-tt^x-1dt,(x)>0

lnη=α₀+α₁ \frac{1}{T} =-9.366 25+6 075.11 \frac{1}{T}