deletions | additions       diff --git a/subsubsection_Johnson_noise_in_1K__.tex b/subsubsection_Johnson_noise_in_1K__.tex  index d213099..59d125c 100644  --- a/subsubsection_Johnson_noise_in_1K__.tex  +++ b/subsubsection_Johnson_noise_in_1K__.tex 
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\subsubsection{Johnson noise in $1K$ Ohm Resistor}  Our settings for the Noise Fundamentals devices were as follows: $1K$ ohm $1K \Omega$  resistor, we used a Gain 1 (G1) of $600$ $\times600$  for all values that comes directly from the Noise Fundamental device, a Gain 2 (G2) of $1000$ $\times1000$  for all values, we used a room temperature of $296.15$ degrees Kelvin, and we varied the high and low pass filters' frequency for each data set in order to vary the bandwidth. In Table 1, you can see how we varied the low pass filter (f2) and the high pass filter (f1) in order to change the bandwidth. The values are taken from the multi-meter after going through the filters, gain, and multiplier - passing through the $A \times A$ multiplier and then being divided by 10 Volts. All of the values are in mV; we took $36$ sets of data points. You can see all these values in \ref{table:Johnson2}. The values in \ref{table:Johnson2} are explained by the following equation: