So, we have that
"I=\\langle S \\rangle=1300 watt\/m^2"
"S=EH"
where
"E=E_0\\cos(\\omega t-kx)"
and
"H=H_0\\cos(\\omega t-kx)"
"S=E_0H_0\\cos^2(\\omega t-kx)"
"\\langle S\\rangle=\\frac{1}{2}E_0H_0"
"E_0\\sqrt{\\epsilon \\epsilon_0}=H_0\\sqrt{\\mu \\mu_0}\\to H_0=\\sqrt{\\frac{\\epsilon_0}{\\mu_0}}E_0"
Finally
"I=\\frac{1}{2}E_0\\sqrt{\\frac{\\epsilon_0}{\\mu_0}}E_0=\\frac{1}{2}E_0^2\\sqrt{\\frac{\\epsilon_0}{\\mu_0}}\\to E_0=\\sqrt{2I\\sqrt{\\frac{\\mu_0}{\\epsilon_0}}}"
So,
"E_0=\\sqrt{2I\\sqrt{\\frac{\\mu_0}{\\epsilon_0}}}=\\sqrt{2\\cdot 1300\\sqrt{\\frac{4\\cdot 3.14\\cdot 10^{-7}}{8.85\\cdot 10^{-12}}}}=990 \\frac{V}{m}"
The End!
Comments
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It is really good.Please expand the middle terms of above example..
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