Patent Description:
Particulate matter such as fine and ultrafine particles (e.g. PM <NUM> or <NUM>) constitute a form of air pollution that may induce adverse health effects on the human body. Particle sensors can be used to measure the concentration of particulate matter and provide information about the air quality. Additionally or alternatively they may also be used as an input for controlling measures that can improve the air quality. For example, a particle sensor can be used in the heating, ventilation and air conditioning (HVAC) system of a car to measure the concentration of hazardous particles in the air flow that is passing through such a system. Based on the information, the system may be configured to reduce the exposure of occupants to air having a low air quality, for instance by controlling the source from which inlet air is sourced or by removing particulate matter from the air stream provided at the inlet.

<CIT> describes such a particle sensor that can be used in combination with an HVAC system. The disclosed particle sensor comprises a set of two flow fans arranged to adjust flow rates in the sensor such that the measurements become largely independent of non-stationary environmental conditions. Therefore, such a sensor system is ideally suitable to sense mass concentrations accurately in an environment where the sampled air is not stationary, like in a moving vehicle or in an HVAC system of a vehicle.

The disadvantage of such a sensor is however that it does not allow to control absolute flow speeds. Consequently, it does not allow complete compensation of the non-stationary environmental conditions such as pressure differences, which results in a reduced accuracy of the measurements. Furthermore, fast changing pressure differences caused in HVAC systems for example by opening a window, activating a blower fan or driving at various speeds easily induces a pressure difference in the order of ~<NUM> Pa, which place a burden on the compensating capabilities of the flow generating components (e.g. fans) used in such a sensor. In order to enable compensation, the flow or pressure difference must be measured and sufficient fan capability must be provided to compensate for this pressure difference, e.g. the static pressure operation point of the fan is orders of magnitude higher than the external disturbance.

<CIT> and <CIT> disclose samplers for sampling gas from a gas stream.

It is an object of the present invention to provide a sampler device and a particle sensor comprising such sampler device that can be used for sampling any gas (including any gas composition), in particular air (including polluted air, such as an exhaust gas of a combustion engine), in non-stationary environmental conditions, in particular from a flow of the gas to be sampled, in particular where the flow rate of the gas to be sampled can vary. It is an aim of the present invention to provide such devices which have an improved efficiency and accuracy in non-stationary environmental conditions. A reference to air in the remainder of the description may be substituted with any gas, unless it specifically relates to air (e.g. a physical parameter of air).

According to the present invention, there is therefore provided a sampler device as set out in the appended claims and a use of such sampler device. According to another aspect, there is provided an assembly or device for sensing particle concentration in air as set out in the appended claims. According to yet another aspect, there is provided a ventilation system as set out in the appended claims. According to yet another aspect, there is provided a vehicle as set out in the appended claims.

A sampler device according to the invention comprises a first chamber through which air from the external environment is made to flow. A second chamber can be fluidly connected to the first chamber. The second chamber can form a sampling chamber and can comprise a particle concentration sensor. The present invention provides a solution to providing a sample air stream by appropriately positioning the inlet and the outlet of the sample air duct in an environment where the air flow velocity can vary drastically on short length and time scales, the pressure difference between the inlet and outlet however remaining small and/or substantially stationary, preferably near zero.

To this end, the first chamber comprises a first inlet and a first outlet and defines a main flow direction between the inlet and the outlet. The first chamber is advantageously placed in an air flow, and an air stream is made to enter the first chamber through the first inlet and exit the first chamber through the first outlet. The first chamber further comprises a second inlet and a second outlet configured to provide respectively a sink and a source of a sample air stream for a particle concentration sensor. The sample air stream is sampled from the first chamber, in particular from the air stream passing through the first chamber, wherein the sample air stream forms a flow through the second outlet. The second inlet and the second outlet are provided in the first chamber at a first position and a second position respectively, which overlap along the main flow direction. In other words, the second inlet and the second outlet are located such that a plane perpendicular to the main flow direction crosses both the second inlet and the second outlet. Advantageously, the second inlet and the second outlet fluidly communicate with a second chamber and may form a closed system from second outlet to second inlet for sample air being sampled from the first chamber. A particle concentration sensor can be housed in the second chamber.

Sampler devices according to the invention provide a solution to providing a stable stream of sample air by appropriately positioning the second inlet and the second outlet of the second chamber in an environment where the air flow velocity can vary drastically on short length and time scales. Therefore, the second inlet and the second outlet are arranged at positions that overlap along the main flow direction of the air that is being sampled from the first chamber. The result is that the second inlet and outlet are subjected to substantially the same environmental conditions. Preferably, the first position and the second position within the first chamber are selected such that a pressure in the first chamber at the first and second positions is substantially equal, thereby minimizing the pressure differences across the inlet and the outlet and reducing influences on the flow of the sample air stream, that may be induced by convection means such as air displacement means. For instance, the first chamber is configured to comprise a plane of symmetry parallel to the main flow direction, and wherein the second inlet and the second outlet are arranged at opposite sides of the plane of symmetry. Such second inlet and second outlet may further comprise an inlet duct and an outlet duct, respectively, adjacent the first chamber and in fluid communication with the first chamber. The inlet duct and outlet duct may be configured in mirror symmetry with respect to the plane of symmetry. Additionally or alternatively, the inlet and outlet duct may each define a longitudinal axis substantially perpendicular to the main flow direction.

The sampler device comprises a second chamber fluidly coupled to the second inlet and to the second outlet, and convection means such as an air displacement means configured to create an air stream from the second outlet to the second inlet through the second chamber. A surprising benefit of a sampler device according to the present invention is that it enables the use of low power flow generating components as convection means such as flow fans, heating means or even ionic motors to maintain the sample air stream from the second outlet to the second inlet. Furthermore, it does not depend on an active system controlling the flow generating components and is therefore robust and does not require additional components like pressure sensors and controllers to compensate or regulate the flow for instance to keep it stable. The sampler device comprises a second chamber fluidly coupled to the second inlet and to the second outlet, and air displacement means configured to create an air stream from the second outlet to the second inlet through the second chamber.

Preferably, the first chamber of the sampler device is configured for providing a laminar flow of the air stream at the first position and the second position. Providing such a laminar flow has the benefit that it allows for creating a more stable air pressure difference, preferably substantially zero, between the second inlet and the second outlet.

A laminar air flow is determined by the flow velocity for a given channel size and geometry and is only to a small extent dependent on air pressure/temperature via the gas viscosity v. For certain applications in HVAC systems of a vehicle the range of pressure and temperature relevant for the gas viscosity may be expected to be between <NUM>,<NUM> and <NUM>,<NUM> bar and between -<NUM> and <NUM> degrees Celsius, respectively. For designing a sampler device, one may choose to evaluate the flow regime using the gas viscosity at standard pressure and temperature conditions (<NUM>. 325kPa; <NUM>). The occurrence of a laminar flow regime for a 'fully developed' flow through a duct is usually indicated by the Reynolds number when: <MAT> In the above equation, the following variables are used: flow velocity v<NUM> (m/s), flow rate Q (m<NUM>/s), characteristic length L (m), duct area A (m<NUM>) and kinematic viscosity v (m<NUM>/s). The (mean) flow velocity of air through the first chamber is governed by the flow rate through the chamber in combination with the (cross sectional) area (v<NUM> = Q/A) of the chamber. The cross sectional area of the first chamber is advantageously evaluated for a section perpendicular to the main flow direction at the position of the second inlet and second outlet. The characteristic length L represents a typical dimension in a fluid flow. In case of a circular shaped tube, the diameter of the tube is defined as the characteristic length. In case of non-circular cross sectional shapes of the first chamber, a hydraulic diameter DH is advantageously used as diameter, i.e. <MAT>, with A cross sectional area (duct area as defined above) and P the wetted perimeter.

Preferably the first chamber has a geometry configured for providing the laminar flow of the air stream at the first position and the second position. For instance, the first chamber has a characteristic length and a duct area configured for providing the laminar flow at a predetermined flow rate or a range of predetermined flow rates of the air stream through the first chamber for instance between about <NUM> an <NUM> lpm, for instance between about <NUM>,<NUM> and <NUM> litre per minute (lpm), for instance about <NUM> lpm. Preferably, the first chamber has a characteristic length and a duct area configured for providing the laminar flow for mean flow velocities through the first chamber ranging for instance between about <NUM> to <NUM>/s, for instance between <NUM> and <NUM>/s. Preferably, the Reynolds number for the air stream is <NUM> or less at the first position and the second position, preferably wherein the Reynolds number is <NUM> or less, preferably <NUM> or less. Preferably, the duct area of the first area lies essentially between <NUM> and <NUM><NUM>, for instance between <NUM> and <NUM><NUM>.

The effect of flow distortions in the first chamber on the pressure difference between the second inlet and the second outlet can be reduced by configuring the sampler to provide a larger flow rate through the first chamber than through the second inlet or the second outlet. Preferably, the predetermined flow rate of the air stream is at least <NUM> times larger than a flow rate of the sample air stream, preferably at least <NUM> times larger, preferably at least <NUM> times larger.

The second inlet and/or the second outlet may be provided in a wall of the first chamber. This can have the advantage that the second inlet and/or the second outlet do not disturb the air stream in the first chamber, in particular the air stream at the first and second position, respectively. Beneficially, the second inlet and/or the second outlet are provided in the wall of the first chamber and are configured for maintaining a laminar flow.

Advantageously, the dimensions and locations of the second inlet and second outlet of the sampler device are arranged such that there is no re-sampling of particle laden air drawn from the first chamber and/or that no large foreign objects can enter the second outlet and/or the second inlet.

In an advantageous embodiment, the first chamber is configured for preventing the sample air stream or a part thereof flowing out of the second inlet into the first chamber from entering the second outlet, for instance for essentially preventing particles (e.g. PM <NUM> or PM <NUM>) comprised in the sample air stream flowing out of the second inlet into the first chamber from entering the second outlet. For instance, the second inlet and the second outlet are configured to have a geometry, size and location in the first chamber that prevents such re-sampling at the predetermined flow rates or flow velocities. Suitable geometries, sizes and locations may be determined using techniques, such as particle and flow finite element method simulations, known to the person skilled in the art. Additionally or alternatively, a (physical) barrier (e.g. baffle) may be arranged between the second inlet and second outlet. While the placement of the second inlet and outlet as defined above will generally avoid re-sampling, placing the second inlet and second outlet close to each other may in some designs introduce the possibility of re-sampling, where (a part of) the particle-laden air flow that is exhausted from the second inlet may re-enter through the second outlet. This re-sampling can advantageously be prevented by providing a (physical) barrier in the first chamber, such as a baffle in between the second inlet and second outlet, where an external air flow ensures that the dust-laden air flow exiting the second inlet is removed in a direction away from the second outlet. Preferably, such baffle extends parallel to the plane of symmetry of the first chamber, even more preferably such baffle defines a plane of symmetry coinciding with the plane of symmetry of the first chamber. Additionally or alternatively, such baffle may extend between opposing walls of the first chamber, thereby creating separate conduits in the first chamber along the main flow direction, one of which conduits comprising the second outlet and another one of the conduits comprising the second inlet.

Advantageously, large foreign bodies (e.g. crumbled leaves, bugs, large pollen) are prevented from entering the second outlet and/or second inlet for instance when switching off the sampler device. Therefore, it is preferred that the second inlet and/or second outlet define an inlet flow direction through the second inlet and/or an outlet flow direction through the second outlet, respectively, wherein the inlet flow direction has a directional component corresponding to gravity (G) and/or the outlet flow direction has a directional component opposite to gravity (G). This may be achieved by arranging the second inlet and/or second outlet in a top wall of the first chamber, the top wall being defined as a wall in which gravity acts in a direction from the top wall towards the interior of the first chamber. These large foreign bodies could potentially block or limit the flow of air in certain parts of a particle concentration sensor, limiting sensor reliability and lifetime. Embodiments wherein the second outlet is provided in the top wall of the first chamber, have the additional advantage that the risk of polluting or damaging the sensor is reduced.

Advantageously, it will be convenient to note that the proposed invention allows for cascading chambers of sample air. By way of example, one or more additional chambers can be provided upstream of the first chamber in a cascaded arrangement. Advantageously, each downstream chamber in the cascade can be connected to an upstream chamber in the same way as the second chamber is connected to the first chamber, e.g. with a respective second inlet and second outlet arranged at overlapping positions along a main flow direction of the upstream chamber, and so forth. The particle concentration sensor is provided in the second chamber advantageously being a last chamber of the cascade, or any subsequently cascaded chamber, advantageously the most downstream chamber of the cascade. Such a cascaded arrangement enhances the total effect of flow stability, for instance by reducing the influence of external pressure fluctuations on the flow rate between the first and second chamber. This allows even the use of an ion motor (with only a few Pa of pressure head) to cope with external pressure variations that normally can be handled only by a pump.

Such a sampler device may comprise a nozzle upstream of the first chamber, for instance configured as a part of a conduit for a flow of an HVAC system. The nozzle comprising a third chamber comprising a third inlet and a third outlet and defining a second main flow direction between the third inlet and the third outlet of a gas stream upstream from the stream in the first chamber. The nozzle further comprises a fourth outlet in fluid communication with the first inlet, e.g. through a first duct connecting the fourth outlet to the first inlet and a fourth inlet in fluid communication with the first outlet, e.g. through a second duct connecting the fourth inlet to the first outlet. The fourth inlet and the fourth outlet are provided in the third chamber at a third position and a fourth position respectively, wherein the third position and the fourth position overlap along the second main flow direction. Such nozzle is configured for flow rates larger than the flow rate through the first chamber, for instance for flow rates between about <NUM> and <NUM> Ipm.

The present invention also relates to a device for sensing particle concentration in a gas, preferably air. Such device for sensing particle concentration comprises a sampler device according to the present invention and a particle concentration sensor in fluid communication with the first inlet and the first outlet, in particular in fluid communication with the first inlet and the first outlet via the second inlet and the second outlet such that the particle concentration sensor senses a particle concentration in the sample gas stream, preferably wherein the sensed particle concentration is representative of the particle concentration in the gas stream between the first inlet and the first outlet.

The present invention further relates to an assembly for sensing particle concentration in a gas. Such an assembly may comprise two devices for sensing particle concentration in a gas, preferably air, wherein each one of the two devices is configured for sampling gas from a different environment, preferably one of the two devices for sampling inside air and the other one of the two devices for sampling outside air. The benefit is that such an assembly may provide information simultaneously regarding a particle concentration in each of the two environments, which information may be used for selecting a source for ventilating a room or a compartment or a cabin for instance housing people or a driver or passengers. As an example, the source comprising the least amount of particles, that may be detrimental to the health, may be selected as a source for the ventilation.

The present invention further relates to a ventilation system for air (e.g. of a vehicle) comprising a sampler device, a device for sensing particle concentration or an assembly according to the present invention.

The present invention further also relates to a vehicle comprising a sampler device, a device for sensing particle concentration, an assembly or a ventilation system according to the present invention.

A use of the sampler device, the device for sensing particle concentration or the assembly according to the present invention for sampling gas (air) is described herein. The sampler device is used under conditions in which a laminar flow is provided in the first chamber, for instance a flow rate of the gas through the first chamber is between about <NUM> an <NUM> Ipm, for instance between about <NUM> and <NUM> Ipm, for instance about <NUM> Ipm. Preferably, the sampler device is used under conditions providing the laminar flow, for instance for mean flow velocities through the first chamber ranging between about <NUM> to <NUM>/s or between <NUM> and <NUM>/s. Preferably, the sampler device is used under condition wherein the Reynolds number for the air stream is <NUM> or less at the first position and the second position, preferably wherein the Reynolds number is <NUM> or less, preferably <NUM> or less.

Referring to <FIG>, a device <NUM> for sensing particle concentration in air comprises a sensor chamber <NUM>, an inlet <NUM> and an outlet <NUM> both fluidly communicating with the sensor chamber <NUM>. A particle concentration sensor <NUM> is housed in the sensor housing <NUM> in order to measure a particle concentration in the flow passing between inlet <NUM> and outlet <NUM>. An air flow <NUM> comprising particles enters device <NUM> through the inlet <NUM>, passes through an air sampler <NUM> and is discharged through the outlet <NUM>. The air flow can be generated or sustained in any suitable way, such as by means of a blower or fan <NUM> which may or may not be arranged between the inlet <NUM> and the outlet <NUM>. The air flow can be externally induced, for instance by placing the air sampler <NUM> in a flow, for instance induced by a fan of an HVAC system. Alternatively, the device can be placed in the environment and natural forces, such as the wind is exploited to create an air flow through the air sampler <NUM>, or the device can be made to move through the environment.

Any suitable kind of sensor can be used as particle concentration sensor <NUM> in devices of the present invention. Advantageously, optical sensors are used, able to measure a particle concentration, e.g. through diffraction of a light beam, such as a laser beam, that is aimed at the air flow. Alternatively, electrostatic particle sensors can be used.

The air sampler <NUM> according to the invention comprises a first chamber <NUM> fluidly coupled between the inlet <NUM> and the outlet <NUM>. The first chamber fluidly communicates with the sensor chamber <NUM> through an inlet <NUM> and an outlet <NUM>. Outlet duct <NUM> connects the outlet <NUM> with the sensor chamber <NUM> and provides sample air to the sensor chamber. Inlet duct <NUM> connects the inlet <NUM> with the sensor chamber and is configured to remove sample air that has passed the sensor chamber <NUM>.

Referring to <FIG>, the first chamber <NUM> comprises at one end an inlet duct <NUM> which can be fluidly coupled to the inlet <NUM> of device <NUM>. The first chamber <NUM> also comprises an outlet duct <NUM> advantageously arranged at the opposite end of the first chamber. Outlet duct <NUM> can be fluidly coupled to the outlet <NUM>. Inlet <NUM> and outlet <NUM> are configured to provide a flow of sample air, sampled from the first chamber <NUM> to the sensor chamber <NUM> where it can be sensed by particle sensor <NUM>, and back to the first chamber <NUM>.

Particle laden air is made to flow from the inlet duct <NUM>, through the first chamber <NUM> to the outlet duct <NUM>, along a main flow direction <NUM>. The inlet <NUM> and outlet <NUM> are arranged in the first chamber <NUM>, in the flow path between inlet duct <NUM> and outlet duct <NUM>. A representative portion of air flowing through the first chamber <NUM> enters the outlet <NUM>, which reconnects to the inlet <NUM> after leaving the sensor chamber <NUM>.

According to the invention, the inlet <NUM> and the outlet <NUM> are arranged at overlapping positions along the main flow direction <NUM>, as depicted schematically in <FIG>.

Referring to <FIG>, the overlapping positions of inlet <NUM> and outlet <NUM> are advantageously arranged next to one another when regarded in a plane perpendicular to the main flow direction <NUM>. At these positions, advantageously, a static and/or dynamic pressure is almost equal, and advantageously no pressure difference exists between inlet <NUM> and outlet <NUM>. As a result, the flow through the sensor chamber <NUM>, and hence the flow that is seen by the particle concentration sensor <NUM>, is not affected by pressure variations at the inlet <NUM> or outlet <NUM>, or in the first chamber <NUM>. Advantageously, the flow of sample air from the outlet <NUM>, through sensor chamber <NUM> to the inlet <NUM> is maintained by a second fan <NUM> (see <FIG>), which can be housed anywhere along the sample air flow path, between outlet <NUM> and inlet <NUM>, in particular in the sensor chamber <NUM>. Fan <NUM> can hence operate independently of fan <NUM>.

The geometry of the first chamber <NUM> is advantageously chosen such that the air flow is smooth/laminar and/or the air flow velocity at the inlet <NUM> and outlet <NUM> is equal. This reduces pressure differences between inlet <NUM> and outlet <NUM>. Furthermore, a laminar flow can reduce the mixing of air flowing out of the inlet <NUM> into the first chamber <NUM> with the air flowing from the first chamber <NUM> into the outlet <NUM>.

In <FIG>, possible design parameters at the inlet <NUM> and outlet <NUM> are indicated. The apertures of inlet <NUM> and outlet <NUM> have respective length L<NUM> and width W<NUM>, and are spaced apart by a distance D<NUM>. The inlet <NUM> and outlet <NUM> are arranged in a wall <NUM> of the first chamber <NUM>, and interposed between opposing walls <NUM> and <NUM>'. A distance between each of the inlet <NUM> and the outlet <NUM> and the corresponding wall <NUM>, <NUM>' is represented by W<NUM>. H represents the chamber height, between wall <NUM> in which inlet <NUM> and outlet <NUM> are arranged and an opposite wall.

The first chamber <NUM> is advantageously symmetric as depicted by the symmetry axis s, but this is not a necessity. The symmetry axis s is parallel to the main flow direction <NUM> and advantageously runs halfway between the inlet <NUM> and the outlet <NUM>. The symmetry axis s advantageously defines a symmetry plane S that comprises the symmetry axis s. The first chamber <NUM> is advantageously symmetrical with respect to the symmetry plane S, and the inlet <NUM> and outlet <NUM> are advantageously located at opposite sides of the symmetry plane S and symmetrical with respect to S. Advantageously, the inlet <NUM> and outlet <NUM> are coplanar and the symmetry plane S is perpendicular to the plane defined by inlet <NUM> and outlet <NUM>, i.e. perpendicular to a plane of the apertures of inlet <NUM> and outlet <NUM>. It will be convenient to note that the dimensions of the inlet <NUM> and outlet <NUM> are advantageously equal, e.g. outlet <NUM> and inlet <NUM> have equal L<NUM> and/or equal W<NUM>.

The air flow is advantageously laminar at the inlet <NUM> and outlet <NUM>, and advantageously in the entire first chamber <NUM>.

Advantageously the flow through the first chamber <NUM> is characterised by Re ≤ <NUM>, advantageously Re ≤ <NUM>, advantageously Re ≤ <NUM>, advantageously Re ≤ <NUM>, and the chamber geometry and flow rate through the first chamber can be selected to achieve the indicated Reynolds number. In determining the Reynolds number, the width W of the first chamber <NUM> at the location of the inlet <NUM> and outlet <NUM> perpendicular to the main flow direction <NUM> can be considered as the characteristic flow dimension. The kinematic viscosity can be evaluated at standard pressure and temperature conditions (<NUM>. 325kPa; <NUM>).

Advantageously, a mean flow velocity through the first chamber <NUM> is <NUM> (m/s) or less, given that W ≈ <NUM> (mm), H ≈ <NUM> (mm) and Q ≈ <NUM> (lpm - litre per minute). This means that the worst-case Reynolds number (when considering a rectangular cross section and L = DH) for standard temperature and pressure (at STP conditions) equals Re = <NUM>, which is well within the range of the laminar flow regime. The flow rate or flow velocity can be selected by appropriate dimensioning of the blower or fan <NUM>.

It will be convenient to note that the outlet <NUM> can be designed to act as a virtual impactor by appropriate design of the outlet geometry and selection of the flow speeds. This can reduce pollution of the particle sensor as it prevents unwanted particles to enter the measurement chamber.

Although a laminar flow of air is advantageously made to enter the first chamber <NUM>, the side walls <NUM> and <NUM>' are placed at a distance W2 from the outlet <NUM> and inlet <NUM> respectively, such that the effect of wall friction on the laminar flow is negligible at the inlet and outlet. This is because end effects such as wall friction may induce small scale turbulent behaviour due to material roughness/imperfections, even in case the air flow can be classified as strictly laminar.

In some circumstances, there can be flow distortions of various kinds causing a non-equal pressure between inlet <NUM> and outlet <NUM>. The effect of such flow distortions on the pressure in the location of the inlet <NUM> and outlet <NUM> can be significantly reduced when the distance D<NUM> is kept sufficiently small such that D<NUM> < W2 <NUM>. In addition, or alternatively the above effect can be reduced when the flow rate through the inlet <NUM> and outlet <NUM> (Q<NUM>) is much smaller than the flow rate through the first chamber (Q<NUM>), for instance Q<NUM> ≥ <NUM> Q<NUM>, advantageously Q<NUM> ≥ <NUM> Q<NUM>.

In general, for accurately measuring particle concentrations it is advantageous when the first chamber is configured for preventing the sample air stream or a part thereof flowing out of the second outlet into the first chamber from entering the second inlet. Thus, on the one hand the distance D<NUM> is advantageously as small as possible to minimize pressure differences between the inlet and outlet of the second chamber, while on the other hand the distance D<NUM> is advantageously sufficiently large to prevent the recirculation of air entering the first chamber from the inlet and re-exiting through the outlet, which may induce erroneous measurements. Preferably, D<NUM> ≥ W<NUM> because this provides sufficient time for outflowing particles to move away before having the possibility to re-enter.

Alternatively or additionally, in order to prevent recirculation in situations where distance D<NUM> is small, a physical barrier, such as a baffle, is placed between the inlet <NUM> and outlet <NUM> (not shown). The baffle projects from the wall <NUM> where the inlet <NUM> and outlet <NUM> are arranged, into the first chamber <NUM>. Such a barrier does not have to extend to the wall of the first chamber opposite to wall <NUM>. The baffle can be placed along the symmetry plane S and have mirror symmetry with respect to S. When the air flow through the first chamber is laminar, the air flow velocities will be the same on both sides of the barrier. Consequently, there will be no pressure difference due to differences in air flow velocity.

Advantageously, the outlet <NUM> is advantageously placed so that the flow direction through the outlet <NUM> is vertically upward, i.e. the wall <NUM> advantageously forms a top wall of the first chamber <NUM>, i.e. gravity acts in a direction from the top wall <NUM> towards the interior of the first chamber <NUM>. The view of <FIG> therefore can be considered as being upside down. This ensures foreign objects like crumbled leaves, insects etc. are not likely to enter the sensor chamber <NUM> due to their inertia, which effect can further be enhanced by the relatively small flow rate through the outlet <NUM> compared to the (main) flow rate of the first chamber (typically, a <NUM>/<NUM> or less of the main flow rate).

It is possible to arrange multiple air samplers <NUM> in parallel, each communicating to a corresponding sensor chamber <NUM>. With such an arrangement particle concentration can be measured simultaneously in multiple air streams.

Referring to <FIG>, a sample nozzle <NUM> according to the invention acts as an air sampler. Sample nozzle <NUM> is placed in an air stream <NUM>, such as the inlet duct of a vehicle ventilation system. The sample nozzle <NUM> can be cylindrically shaped, although other shapes are possible as well. The sample nozzle <NUM> comprises an inlet side <NUM> arranged at an upstream end of the sample nozzle <NUM> and an outlet side <NUM> arranged at a downstream end of the sample nozzle, advantageously opposite the inlet side <NUM>. The flow through the sample nozzle <NUM> proceeds along main flow direction <NUM>, from the inlet side <NUM> to the outlet side <NUM>, advantageously aligned along, or parallel to a direction <NUM> of the air stream <NUM>. The main flow direction <NUM> is advantageously parallel to an axis of the sample nozzle <NUM>, e.g. a cylinder axis.

Two sample ducts <NUM>, <NUM> have first ends that are connected to the sample nozzle <NUM>, between inlet side <NUM> and outlet side <NUM>. Sample ducts <NUM> and <NUM> have second ends opposite the first ends that are fluidly connected to a sensor chamber (e.g. sensor chamber <NUM> in <FIG>). The first ends of sample ducts <NUM>, <NUM> are arranged in the wall of the sample nozzle <NUM> and respectively form the inlet <NUM> and outlet <NUM>. The inlet <NUM> and outlet <NUM> are advantageously arranged at opposite wall portions of the sample nozzle, at a same or overlapping position along the main flow direction <NUM> through the sample nozzle <NUM>.

A baffle <NUM> is arranged in the sample nozzle <NUM>, splitting it into a first half <NUM> and second half <NUM>. The inlet <NUM> is arranged in a wall portion of the first half <NUM> of sample nozzle <NUM>, whereas the outlet <NUM> is arranged in a wall portion of the second half <NUM> of sample nozzle <NUM>. Baffle <NUM> therefore forms a physical barrier separating the inlet <NUM> and the outlet <NUM>. The baffle <NUM> advantageously extends from a position upstream the location of inlet <NUM> and outlet <NUM>, e.g. from inlet side <NUM>, to a position downstream the location of inlet <NUM> and outlet <NUM>, e.g. to the outlet side <NUM>, when considered along the main flow direction <NUM>. Baffle <NUM> advantageously has a median plane advantageously extending parallel to a major face or wall of the baffle, which forms a plane of symmetry S of baffle <NUM>. This plane of symmetry S advantageously is a plane of symmetry of the entire sample nozzle <NUM>, and inlet <NUM> and outlet <NUM> are advantageously arranged symmetrically with respect to the plane of symmetry S.

Due to the baffle <NUM>, the flow entering sample nozzle <NUM> is split, e.g. at the inlet side <NUM>, in two parts. A first part flows through the first half <NUM> in which the inlet <NUM> is arranged. A second part flows through the second half <NUM> in which the outlet <NUM> is arranged. A portion of the second part of the flow enters the outlet <NUM>, flows through the sample duct <NUM> to the sensor chamber. The first part receives the flow that exits the sensor chamber through the sample duct <NUM>. Advantageously, the flow path forms a closed loop from the outlet <NUM> to the inlet <NUM> through the sensor chamber. With such a configuration, it is ensured that there is almost no pressure difference between the inlet <NUM> and the outlet <NUM> (in particular when a fan <NUM> in the sensor chamber <NUM> is not operating).

Sample air flowing from the sample nozzle <NUM> through the first outlet <NUM> defines an outlet direction <NUM> and sample air flowing through inlet <NUM> back into the sample nozzle <NUM> defines an inlet direction <NUM>. Advantageously, the inlet <NUM> and the outlet <NUM> are arranged symmetrically with respect to the plane of symmetry S of sample nozzle <NUM>. Additionally, the directions <NUM> and <NUM> may advantageously be arranged symmetrical with respect to the plane of symmetry S.

Similar considerations apply to the air flow in the sample nozzle <NUM> as described in relation to <FIG> above. By way of example, the flow regime in the sample nozzle is advantageously laminar.

Referring to <FIG>, the outlet direction <NUM> of sample air flowing through the outlet <NUM> and the inlet direction <NUM> of sample air flowing through the inlet <NUM> back into the sample nozzle are advantageously transverse to, and advantageously substantially perpendicular to the main flow direction <NUM> through the sample nozzle <NUM>. The angle A1 of inlet direction <NUM> and angle A2 of outlet direction <NUM> with respect to the main flow direction <NUM> is advantageously between <NUM>° and <NUM>°, advantageously between <NUM>° and <NUM>°, and advantageously substantially <NUM>°. Preferably, the angles A1 and A2 are essentially the same. A significant deviation from this may lead to a pressure difference between the inlet <NUM> and the outlet <NUM>. In the above a convention is used, in which the angle is determined starting from the upstream side of flow direction <NUM>.

A flow velocity through the inlet <NUM> and/or the outlet <NUM> is typically <NUM> - <NUM>/s for a channel diameter of <NUM> - <NUM>. The flow velocity through the inlet <NUM> and/or the outlet <NUM> is typically much smaller than the flow velocity through the first chamber (sample nozzle <NUM>).

The angles A1 and A2 are advantageously equal (in absolute value) to avoid a significant pressure difference between inlet <NUM> and outlet <NUM> in situations where for instance the flow velocity through the second chamber (e.g. into the inlet <NUM> and exiting the outlet <NUM>) is much smaller than the flow velocity through the first chamber (e.g. the first and second nozzle half <NUM>, <NUM> of sample nozzle <NUM>). Typically, the flow velocity through the sample nozzle can show a large variation, e.g. when placed in communication with an HVAC system, which may induce flow velocities through the first chamber that are in the order of <NUM>/s and may go up to <NUM>/s.

The angles A1 and A2 may however be different, for instance to compensate for a pressure difference induced by the flow through the sample ducts. Additionally or alternatively, the angle A1 can be different from <NUM>° to influence particle sampling behaviour at the inlet <NUM>. For such embodiments it may be advantageous to have a relatively stable flow rate through the sample nozzle.

Referring to <FIG>, the angles A3 and A4 between respectively the inlet direction <NUM> and the outlet direction <NUM> with respect to the plane of symmetry S are advantageously equal (in absolute value) and can be between <NUM>° and <NUM>°, advantageously between <NUM>° and <NUM>°, advantageously between <NUM>° and <NUM>°, advantageously between <NUM>° and <NUM>°, advantageously <NUM>°. Angles A3 and A4 can be <NUM>° or less, e.g. between <NUM>° and <NUM>°, advantageously between <NUM>° and <NUM>°. It will be convenient to note that the inlet <NUM> and outlet <NUM> are advantageously arranged in a top half of the first half <NUM> and second half <NUM> respectively to avoid that debris that is entrained with the air stream <NUM> could fall in the inlet <NUM> or outlet <NUM> by gravity which is indicated in <FIG> by the arrow G.

Advantageous features and considerations (e.g. baffle <NUM>, location of inlet <NUM>, location of outlet <NUM>, inlet direction <NUM>, outlet direction <NUM>, angles A1-A4) for embodiments described above in relation to sample nozzle <NUM> of <FIG> similarly apply to air sampler <NUM> shown in <FIG>.

The sampler device is advantageously designed such that the (mean) flow velocity into the inlet <NUM> or <NUM> and exiting the outlet <NUM> or <NUM> is significantly smaller than the (mean) flow velocity through the first chamber (or sample nozzle). Advantageously a ratio of mean flow velocity through inlet <NUM> or outlet <NUM> to the mean flow velocity through the first chamber <NUM> or sample nozzle <NUM> is <NUM>/<NUM> or less, advantageously between <NUM>/<NUM> and <NUM>/<NUM>, advantageously between <NUM>/<NUM> and <NUM>/<NUM>, advantageously about <NUM>/<NUM>.

In an advantageous embodiment of the sampler device according to the invention, the first chamber <NUM> of <FIG> and the sample nozzle <NUM> of <FIG> are cascaded. In particular, the sample nozzle <NUM> is placed upstream of the first chamber <NUM>, e.g. in an air stream <NUM>, e.g. the ventilation duct of a vehicle or a building, and the inlet <NUM> and outlet <NUM> of the sample nozzle <NUM> are fluidly connected to the outlet <NUM> and the inlet <NUM> respectively of the first chamber <NUM>. The sensor chamber <NUM> can be connected to the inlet <NUM> and the outlet <NUM> of the first chamber <NUM> as shown in <FIG>. By so doing an arrangement is obtained with three cascaded chambers, i.e. the sample nozzle <NUM>, the first chamber <NUM> and the sensor chamber <NUM>. Such an arrangement advantageously allows for further stabilizing the sample air flow through the sensor chamber irrespective of dynamic pressure variations of air stream <NUM>. Such an arrangement also allows for a stepwise reduction in flow rates. For instance, the flow rate through sample nozzle <NUM> may be about <NUM> Ipm, while the flow rate through first chamber <NUM> is about <NUM> Ipm and the flow rate through the sensor chamber is about <NUM> Ipm.

Claim 1:
Sampler device (<NUM>) for sampling gas for a particle concentration sensor from a flow, comprising:
a first chamber (<NUM>, <NUM>) comprising a first inlet (<NUM>) and a first outlet (<NUM>) and defining a main flow direction (<NUM>) of a gas stream between the first inlet and the first outlet, the first chamber comprising a wall in which a second inlet (<NUM>) and a second outlet (<NUM>) are provided,
wherein the second inlet and the second outlet are configured to provide a sink and a source of a sample gas stream, respectively,
a second chamber fluidly coupled to the second inlet and to the second outlet,
gas displacement means provided along the sample gas stream between the second outlet (<NUM>) and the second inlet (<NUM>) and configured to create the sample gas stream from the second outlet to the second inlet through the second chamber,
wherein the second inlet (<NUM>) and the second outlet (<NUM>) are provided in the first chamber (<NUM>, <NUM>) at a first position and a second position respectively, and
wherein the first position and the second position overlap along the main flow direction (<NUM>), characterized in that the sampler device comprises
a baffle (<NUM>) arranged in the first chamber between the second inlet and the second outlet, wherein the baffle projects from the wall into the first chamber.