A common definition for the quality factor \( Q \) around a resonance \( f_0 \) is \[ Q = \frac{f_0}{f_2 - f_1}, \] where \( f_1 \) and \( f_2 \) are the half-power (or \(-3 \, \text{dB}\)) frequencies. Here: \[ f_0 = 300 \, \text{Hz}, \quad f_1 = 150 \, \text{Hz}, \quad f_2 = 450 \, \text{Hz}. \] Thus, \[ f_2 - f_1 = 450 \, \text{Hz} - 150 \, \text{Hz} = 300 \, \text{Hz}, \quad \Rightarrow \quad Q = \frac{f_0}{f_2 - f_1} = \frac{300}{300} = 1.0. \] Hence the quality factor is \fbox{1.0}.
List I | List II |
---|---|
(A) (∂S/∂P)T | (I) (∂P/∂T)V |
(B) (∂T/∂V)S | (II) (∂V/∂S)P |
(C) (∂T/∂P)S | (III) -(∂V/∂T)P |
(D) (∂S/∂V)T | (IV) -(∂P/∂S)V |
Ultraviolet light of wavelength 350 nm and intensity \(1.00Wm^{−2 }\) falls on a potassium surface. The maximum kinetic energy of the photoelectron is