down, the offset advances in larger and larger increments, the largest increment being 10% of full scale. When the offset is turned OFF the applied offset returns to zero but the offset value is not lost. The next press of the upper offset key (return to ON) sets the offset to the previously entered value.

If an attempt is made to advance the offset value beyond full scale, the ON LED will blink. An offset up to 1.024 times the full-scale sensitivity may be entered. When the EXPAND is on, this is 10X the full scale output.

Note that the offsets (either manual offset or those generated by the REL function) represent a fraction of the full scale reading, and so their absolute value will change when the sensitivity scale is changed. A signal which has been nulled by an offset will not be nulled when the sensitivity scale is changed. The analog meter and the output BNC indicate the same value given by the equation:

Vout = 10Ae(AvVisinØ+V os) {if the output is Y}

where...

 

 

Ae

= 1 or 10 per the Expand

Av

=

1/Sensitivity

Vi

=

magnitude of the signal

Ø= phase between signal & reference Vos = offset (fraction of FS < 1.024)

When the DISPLAY is Y, Y OFST, or Y NOISE, the OFFSET keys adjust the Y OFFSET (which affects the Y (RSINØ) output). When the DISPLAY is Ø, the OFFSET keys do nothing. When the DISPLAY is X6, the OFFSET up and down keys set the output voltage of D/A output X6 (also on the rear panel) up to ±10.24V.

Expand Channel 2

The output EXPAND is toggled by pressing the key in the Channel 2 EXPAND section. The expand status is indicated by the X10, expand on, and the X1, expand off, LED's. Only the Channel 2 OUTPUT is affected, the Y (RSINØ) output is not expanded. Ø and X6 may not be expanded.

Y (RSINØ) Output

The analog output, Y+Yofst, is available at the Y (RSINØ) BNC connector. An input signal equal in magnitude to the selected sensitivity which is 90° out of phase with the reference oscillator will generate a 10V output. The output impedance is <1Ω and the output current is limited to 20 mA.

The Y (RSINØ) output is affected by the Y offset but may not be expanded. The Y (RSINØ) is not affected by the DISPLAY setting except for two cases. When the DISPLAY is set to Y OFST, the Y (RSINØ) output is the Y offset. When the DISPLAY is set to Y NOISE, the Y (RSINØ) output has a bandwidth equal to the ENBW (1 or 10 Hz) instead of the time constant.

Reference Input

The REFERENCE INPUT BNC is located in REFERENCE INPUT section. The input is ac coupled and the impedance is 1 MΩ . The dc voltage at this input should not exceed 100 V and the largest ac signal should be less than 10 V peak.

Trigger Level

The TRIGGER MODE indicator toggles from POSITIVE to SYMMETRIC to NEGATIVE when the TRIGGER MODE key is pressed.

If the center TRIGGER MODE LED is on, the mode is SYMMETRIC and the reference oscillator will lock to the positive zero crossings of the ac reference input. The ac signal must be symmetric (e.g. sine wave, square wave, etc.) and have a peak to peak amplitude greater than 100 mV. A signal with 1 Vrms amplitude is recommended. The phase accuracy of the reference channel is specified for a 1Vrms sinewave in the symmetric trigger mode.

If the upper TRIGGER MODE LED is on, the mode is POSITIVE. The trigger threshold is +1V and the reference oscillator will lock to the positive going transitions of the reference input. This mode triggers on the rising edges of a TTL type pulse train. The pulse width must be greater than 1 µ S.

If the lower TRIGGER MODE LED is on, the mode is NEGATIVE. The trigger threshold is -1V and the reference oscillator will lock to the negative

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SRS Labs Lock-In Amplifier, SR530 manual Rsinø Output, Reference Input, Trigger Level

SR530, Lock-In Amplifier specifications

The SRS Labs Lock-In Amplifier, model SR530, is a powerful tool designed for high-precision measurements in the realm of scientific research and industrial applications. This state-of-the-art instrument excels in extracting small signals from noisy environments, making it an invaluable asset for experiments in fields such as physics, engineering, and materials science.

One of the main features of the SR530 is its ability to perform synchronous detection, which is key to improving signal-to-noise ratios. By utilizing a reference signal, the device correlates the incoming signal with the reference to effectively filter out noise, allowing for the accurate measurement of weak signals that might otherwise be obscured. This process of phase-sensitive detection is fundamental to the operation of the Lock-In Amplifier.

The SR530 offers a wide frequency range, covering from 0.1 Hz to 100 kHz. This broad frequency response allows it to handle a diverse array of signals, making it suitable for various applications including optical detection, capacitance measurements, and in many cases, voltammetry. The device is also equipped with multiple inputs and outputs, facilitating the integration with other laboratory equipment and enabling complex experimental setups.

Precision is further enhanced with its adjustable time constant, which allows users to optimize the response time based on experimental needs. The user can choose time constants from 10 microseconds to 10 seconds, accommodating fast dynamic measurements as well as those requiring stability over longer durations.

Another remarkable characteristic of the SR530 is its digital processing capabilities. The device features a highly accurate digital voltage measurement system, minimizing drift and ensuring long-term stability. Additionally, the use of microprocessors enhances data handling and allows for features such as programmable settings, facilitating automated measurements.

Moreover, the SR530 includes a range of output options, including analog outputs, which can be used for direct signal processing, as well as digital interfaces for integration with computers. This ensures that users can not only capture high-fidelity data but also analyze and display it efficiently.

In conclusion, the SRS Labs SR530 Lock-In Amplifier stands out due to its sophisticated technology, versatile features, and robust performance. Its precision, flexibility, and ease of use make it an ideal choice for researchers and engineers looking to unlock the potential of weak signal measurement in complex environments.