139832 At normal incidence, a beam of light propagating in vacuum reflects of an interface with a medium of refractive index \(n=3\). The fraction of energy reflected \(R\) is given as \(R=\left(\frac{n-1}{n+1}\right)^{2}\). If the fractional error in the value of \(n\) is \(1 \%\), the fractional error in the estimation of \(R\) is:
139832 At normal incidence, a beam of light propagating in vacuum reflects of an interface with a medium of refractive index \(n=3\). The fraction of energy reflected \(R\) is given as \(R=\left(\frac{n-1}{n+1}\right)^{2}\). If the fractional error in the value of \(n\) is \(1 \%\), the fractional error in the estimation of \(R\) is:
139832 At normal incidence, a beam of light propagating in vacuum reflects of an interface with a medium of refractive index \(n=3\). The fraction of energy reflected \(R\) is given as \(R=\left(\frac{n-1}{n+1}\right)^{2}\). If the fractional error in the value of \(n\) is \(1 \%\), the fractional error in the estimation of \(R\) is:
139832 At normal incidence, a beam of light propagating in vacuum reflects of an interface with a medium of refractive index \(n=3\). The fraction of energy reflected \(R\) is given as \(R=\left(\frac{n-1}{n+1}\right)^{2}\). If the fractional error in the value of \(n\) is \(1 \%\), the fractional error in the estimation of \(R\) is: