The present invention relates to optical measuring and testing of aerosol samples by particle light scattering, as in a nephelometer instrument, and in particular to reducing DC and parasitic instrument background noise or otherwise separating such noise from the particle scatter signal.
Nephelometer instruments for measuring the mass per unit volume of ambient aerosols have historically used a light source, such as a diode laser or light-emitting diode (LED), to illuminate a view volume containing particles suspended in a gas carrier. The amount of detected optical scatter from the illuminated particles in the view volume has then been taken as a measure indicative of the amount (mass) of particulate material in the aerosol. Continuous or near-continuous, near-real-time monitoring of the mass, for example in ambient air, can be accomplished by continuously or near-continuously sampling the ambient by pulling the particle carrier gas into and through the instrument view volume. The level of the detected optical signal is then at any time an instantaneous indicator of the mass of particles in the view volume.
Electronic signals suffer from what is known as “1/f noise”, contributed for example by the detector. Electronic noise, including the 1/f noise, can be removed or filtered by a technique involving modulation of the light source intensity in time. The amount of light scattered by the illuminated particles in the view volume will thus also be modulated away from a near-DC level. Synchronous detection of the modulated scattering is a sensitive method of separating the modulated scattering signal from the essentially steady level of electronic noise.
Unfortunately, the same detected optical signal also includes a background parasitic scattering from the nephelometer itself, such as scattering from internal optical components or from contaminants within the sensor instruments. Because this parasitic scattering will also be modulated in the same manner as that of the particle scattering, it cannot be separated out by the light modulation technique and forms a background noise level in the instrument underlying the desired particle scatter signal.
What is needed is a nephelometer instrument and noise filtering technique that can not only remove the 1/f or electronic noise, but also the background parasitic scattering contributions of the instrument, so as to obtain a scattering signal that is a more accurate indicator of ambient particle concentration.
The invention is a nephelometer that provides a way to modulate the proportion of ambient sample gas and thus modulate the concentration of particulates that can enter the view volume. Such modulation can be achieved by periodically injecting clean filtered air into the stream of the particle aerosol sample, thereby diluting the particle concentration. Scattering from the particles is modulated synchronously with the proportion of ambient sample gas, while the parasitic instrument scattering is not. The detected scatter signal can then be readily filtered, e.g., with a lock-in amplifier using the sample modulation rate as a reference frequency, so as to separate the synchronously modulated particle signal from the various near-DC or asynchronous contributions of background noise.
The optical source in this nephelometer can operate at a constant output level, i.e. with no modulation. Alternatively, the optical source could still be intensity modulated, e.g. to stabilize the light output against optical-feedback-induced laser noise, but with a modulation frequency much higher than the modulation of the particle concentration. As long as the different forms of modulation have highly disparate and incommensurate frequencies, all of the different noise contributions can be filtered by the synchronous detection technique. A higher signal-to-noise ratio and higher instrument sensitivity results.
With reference to
The nephelometer instrument also comprises a sample concentration modulation mechanism. In the embodiment of
In the absence of such a mechanism, a steady or near-steady flow of sample would be pulled through the view volume. However, when activated, the pump 25 periodically introduces pulses of clean air or other gas through one branch of the junction 29 into the flow, thereby periodically diluting the sample. As a result, the input 31 to the optical sensor unit 11 downstream of the junction 29 contains a concentration-modulated aerosol stream as the relative proportions of sample and clean air vary.
In alternative embodiment, seen in
In either embodiment, the concentration modulation may have an amplitude that swings from all sample to all clean gas (unity modulation depth), or can have lesser modulation depths (non-unity modulation depth) where the concentration varies from all sample to a mixture of sample and clean gas, or from all clean gas to a mixture of sample and clean gas, or from different mixture proportions of sample and clean gas. The non-unity modulation depths would have a reduced signal-to-noise benefit compared to the unity modulation case, so unity modulation depth is preferred.
The detector output 37 or 77 from the optical sensor 11 or 51, representing the detected particle scattering plus noise, is processed in a manner essentially similar to the case of modulated light intensity in order to separate the signal from the noise. In particular, with modulated sample concentration, the particle scattering will modulate according to the relative proportion of sample air. Accordingly, the scattering contribution from the sample can be computed. In particular, the signal processing carried out by the electronics associated with the optical sensor unit 11 or 51 may employ a lock-in amplifier 35 or 75 wherein the detector output 37 or 77 in the sensor unit is mixed with a reference frequency fREF (from oscillator 33 or 73) which is chosen to be the same frequency as the sample concentration modulation rate. Any contribution to the detection signal that is not at the same frequency as the reference frequency will be attenuated essentially to zero by the lock-in amplifier's low pass filter. While any sample modulation profile provided by the diaphragm pump 25 or variable flow valve 66 could be used, the sample modulation will ideally approach a single frequency sinusoidal profile so that signal and noise are separated sufficiently in the frequency domain. As a lock-in amplifier is phase sensitive, the reference frequency fREF may also serve as a variable flow control CTRL for the variable pump 25 or variable flow valve 66, thereby ensuring that the noise filtering by the lock-in amplifier is synchronized with the concentration modulation. The now-filtered detection signal 39 or 79 is output from the lock-in amplifier and may be further processed as in other known nephelometer instruments to obtain particle data for the aerosol sample.
A nephelometer in accord with the invention will provide effective filtering of both 1/f noise and intrinsic instrumental scattering and give a more accurate and more sensitive particle-sensing instrument.
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