Table. \ref{table:Johnson1} shows the values for the Johnson Noise \(<V_J>^2 + <V_{\textrm{instrumentation}}>^2\) in units of Volts\(^2\)from a resistance value of \(10 k \Omega\), a temperature of \(295\) Kelvin, a \(G1\) of \(\times600\), a \(G2\) of \(\times1000\), and we varied the \(f1\) and \(f2\) in order to change the bandwidth.

The values in \ref{table:Johnson1} are explained by the following equation:

\(V_{\textrm{meter}} = (<V_J>^2 + <V_{\textrm{amplifiers}}>^2) G_1 G_2 / (10 \textrm{Volts}) \textrm{ [mV]}\)

where the factor of \(10 \textrm{Volts}\) comes from the amplifier and the \(<V_J>^2 + <V_{\textrm{amplifiers}}>^2\) is the measured voltage from the multi-mete before the error has been subtracted.