The square of this quantity is defined as 2 in Rydberg atomic units. The root-mean-square fluctuation in shot noise equals the square root of 2 times the current times the bandwidth times this quantity. This quantity is equal to 2 divided by the product of the Von Klitzing and Josephson constants, allowing for this quantity
The square of this quantity is defined as 2 in Rydberg atomic units. The root-mean-square fluctuation in shot noise equals the square root of 2 times the current times the bandwidth times this quantity. This quantity is equal to 2 divided by the product of the Von Klitzing and Josephson constants, allowing for this quantity and Planck's constant to be determined using watt balance experiments. This quantity appears squared in the numerators of the expressions for the plasma frequency and the (*) fine structure constant. An experiment to measure this quantity achieved a low result by using an incorrect value for the viscosity of air, which was ionized using X-rays. That experiment measured the terminal velocity of drops of oil and was performed by Robert Millikan. For 10 points, name this constant equal to minus 1.602 times 10 to the minus 19 Coulombs.
The square of this quantity is defined as 2 in Rydberg atomic units.