365269
The band gap in germanium is \({E}_{{g}}=0.64 \,{eV}\). Assuming that the number of hole-electron pairs is proportional to \({e}^{\left(-{E}_{{g}} / 2 k {~T}\right)}\), find the fractional increase in the number of charge carriers in pure germanium as the temperature is increased from \(300 {~K}\) to \(384 {~K}\).
[Take \({k = 1.4 \times {{10}^{ - 23}},\ln (14.4) = \frac{8}{3}}\)]
365269
The band gap in germanium is \({E}_{{g}}=0.64 \,{eV}\). Assuming that the number of hole-electron pairs is proportional to \({e}^{\left(-{E}_{{g}} / 2 k {~T}\right)}\), find the fractional increase in the number of charge carriers in pure germanium as the temperature is increased from \(300 {~K}\) to \(384 {~K}\).
[Take \({k = 1.4 \times {{10}^{ - 23}},\ln (14.4) = \frac{8}{3}}\)]
365269
The band gap in germanium is \({E}_{{g}}=0.64 \,{eV}\). Assuming that the number of hole-electron pairs is proportional to \({e}^{\left(-{E}_{{g}} / 2 k {~T}\right)}\), find the fractional increase in the number of charge carriers in pure germanium as the temperature is increased from \(300 {~K}\) to \(384 {~K}\).
[Take \({k = 1.4 \times {{10}^{ - 23}},\ln (14.4) = \frac{8}{3}}\)]
365269
The band gap in germanium is \({E}_{{g}}=0.64 \,{eV}\). Assuming that the number of hole-electron pairs is proportional to \({e}^{\left(-{E}_{{g}} / 2 k {~T}\right)}\), find the fractional increase in the number of charge carriers in pure germanium as the temperature is increased from \(300 {~K}\) to \(384 {~K}\).
[Take \({k = 1.4 \times {{10}^{ - 23}},\ln (14.4) = \frac{8}{3}}\)]
365269
The band gap in germanium is \({E}_{{g}}=0.64 \,{eV}\). Assuming that the number of hole-electron pairs is proportional to \({e}^{\left(-{E}_{{g}} / 2 k {~T}\right)}\), find the fractional increase in the number of charge carriers in pure germanium as the temperature is increased from \(300 {~K}\) to \(384 {~K}\).
[Take \({k = 1.4 \times {{10}^{ - 23}},\ln (14.4) = \frac{8}{3}}\)]