Yale University

PHYS 381/504: Op. amps., quartz resonators, and noise

Introduction
Johnson Noise
Macroscopic Derivation
Microscopic Derivation
Install and Test the Optical Amplifier
Install the Tuning Fork
Welcome to LabView
Tune out the Package Capacitance
Gather Data
Load the Driven Circuit Data
Fit the Driven Circuit Data
Find Circuit Characteristics from this Fit
Analyze the Undriven Circuit from Characteristics
Final Results
References
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Andrew Pariser, December 2005
modified S.M., January 2006

© 2006 Yale University, New Haven, Connecticut 06520

Johnson Noise

Electronic noise in circuits is often very difficult to combat when one attempts to make measurements to high precision. There are many sources of this electronic noise; here we focus on Johnson Noise.

Johnson Noise (at a given frequency) is dependent upon two variables: the temperature of the system, and the resistivity in the circuit.

Microscopically, the electricity charge carriers (electrons) have some average drift velocity. This average drift velocity is the average of each particle's individual velocity. Each electron's velocity corresponds to some voltage per electron; even though there is an average current, there is some variability in the individual particles current, providing a variability in the output power (voltage squared).

Even without driving a circuit with any voltage, one will be able to observe this Johnson Noise, which happens to occur on a wide frequency spectrum.

We derive the expression for Johnson Noise, Johnson Noise Equation, in two different ways on the next two pages.

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