Aerosol-generating device and system comprising a pyrometer
11644365 · 2023-05-09
Assignee
Inventors
- Michel Bessant (Neuchatel, CH)
- Jacques Robert (Le Mont-sur-Lausanne, CH)
- Riccardo Riva Reggiori (St. Sulpice, IT)
- Alexandru Rusu (Lausanne, CH)
- Peter Seitz (Urdorf, CH)
Cpc classification
B05B12/004
PERFORMING OPERATIONS; TRANSPORTING
B05B12/10
PERFORMING OPERATIONS; TRANSPORTING
G01J5/06
PHYSICS
International classification
B05B12/00
PERFORMING OPERATIONS; TRANSPORTING
B05B12/10
PERFORMING OPERATIONS; TRANSPORTING
G01J5/06
PHYSICS
Abstract
The present invention relates to an aerosol-generating device that is configured for generating an inhalable aerosol by heating an aerosol-forming substrate. The device comprises a device housing for receiving the aerosol-forming substrate and a pyrometer for determining a temperature of a heated target surface within the device housing. The invention further relates to an aerosol-generating system comprising such an aerosol-generating device and an aerosol-generating article for use with the device including an aerosol-forming substrate.
Claims
1. An aerosol-generating device configured for generating an aerosol by heating an aerosol-forming substrate, the device comprising a device housing for receiving the aerosol-forming substrate, and a pyrometer for determining a temperature of a heated target surface within the device housing, wherein the pyrometer is a dual-wavelength pyrometer or a multiple-wavelength pyrometer that is configured to measure thermal radiation at least at a first wavelength band and a second wavelength band, wherein the second wavelength band is broader than the first wavelength band, and wherein the pyrometer includes a detector comprising at least a first and a second sensor, wherein the first and the second sensor are arranged adjacent to each other side by side, and wherein the pyrometer comprises an optical system for collecting thermal radiation emitted from the heated target surface, wherein the optical system comprises a lens having a lens surface far side of the target surface which is a scattering surface.
2. The device according to claim 1, further comprising an optical shielding for shielding the pyrometer from ambient light.
3. The device according to claim 1, wherein a first optical bandpass or longpass or shortpass filter is arranged in front of the first sensor.
4. The device according to claim 1, wherein a second optical bandpass or longpass or shortpass filter is arranged in front of the second sensor.
5. The device according to claim 1, wherein the detector comprises at least a third sensor.
6. The device according to claim 5, wherein a spectral sensitivity of the third sensor is different from a spectral sensitivity of the first and second sensor.
7. The device according to claim 5, wherein the detector comprises at least a fourth sensor.
8. The device according to claim 7, wherein a spectral sensitivity of the fourth sensor is different from a spectral sensitivity of the first and second sensor.
9. The device according to claim 7, wherein a third optical bandpass filter is arranged in front of the third sensor and a fourth optical bandpass filter is arranged in front of the fourth sensor, and wherein a wavelength band of the third bandpass filter is different from a wavelength band of the fourth bandpass filter.
10. An aerosol-generating system comprising an aerosol-generating device according to claim 1 and an aerosol-generating article for use with the device comprising an aerosol- forming substrate.
11. The system according to claim 10, wherein the device comprises a heater for generating heat in a heating element that is arranged or arrangeable within the aerosol- forming substrate of the article, and wherein the heating element comprises the heated target surface.
Description
(1) The invention will be further described, by way of example only, with reference to the accompanying drawings, in which:
(2)
(3)
(4)
(5)
(6)
(7)
(8) Of course, the device according to
(9) The device 1 further comprises an electrical circuitry 20—powered by a battery 10—which is configured, inter alia, for generating the alternating driving current. The electrical circuitry 20 comprises a controller (not shown) for controlling the heating process.
(10) Controlling the heating temperature requires temperature monitoring of the heating element 32. For this, the device 1 according to
(11) As can be further seen from
(12) Further details of the dual-wavelength pyrometer 100 are described below with regard to the embodiments shown in
(13)
(14) Of course, the device according to
(15) For measuring the absolute temperature of the mesh-susceptor 232, the device 1 according to
(16) In both embodiments according to
(17)
(18) Dual-wavelength pyrometry requires measuring the thermal radiation emitted by the target surface at two wavelength or wavelength bands. In the present embodiment, this is accomplished by using a longpass filter 131 arranged in front of the first sensor 121 only. The longpass filter 131 has a cut-off wavelength of 1.6 micrometer. InGaAs is sensitive for wavelengths between 0.9 micrometer and 1.7 micrometer. Thus, the cut-off wavelength of the longpass filter 131 and the long-wave end of the spectral sensitivity range of the InGaAs sensor 121 provide an effective bandpass filtering of the thermal radiation sensed by the first sensor 121 to the range of 1.6 micrometer to 1.7 micrometer. In contrast, the second sensor 122 has no filter in front and thus monitors the full spectral band according to the sensitivity of InGaAs in the range of 0.9 micrometer to 1.7 micrometer. Hence, due to the cut-off wavelength of the longpass filter 131, a difference between the output signals of the first and second sensor 121, 122 is achieved which is reasonably measurable and thus well suited for determining the temperature of the heated target surface 33, 233 as described above.
(19) As further described above, at least the second sensor 122 needs to be manually calibrated across the full wavelength spectrum. This can be done for example by using a blackbody emitter at different known temperatures of the black body. The first sensor 121 may be also calibrated in the same way. In principle, once the initial calibration is made, the emissivity of the target surface 33, 233 does not need to be known any longer (in case the target surface 33, 233 is a grey body). In the case that the target surface is a non-grey body, a second calibration should be made taking into account the variation of emissivity. This calibration needs to be done only for one device of a specific type.
(20) Advantageously, the dual-wavelength pyrometer 100 is inherently accurate as it allows not only for compensating for emissivity variations, but also for partially filled fields of view and optical obstructions between the target surface and the detector of the pyrometer.
(21) For collecting thermal radiation emitted from the heated target surface 33, 233 and for directing the thermal radiation towards the detector 120, the dual-wavelength pyrometer 100 comprises an optical system 110. In the present embodiment, the optical system 100 comprises two lenses, a converging lens 114 and a semi-convex lens 111. The optical system 100 provides a field of view on the target surface 33, 233 having a diameter of at least 1 millimeter.
(22) In use of the aerosol-generating device 1, aerosol particles and droplets 300 may accumulate on the front surface of the optical system 120 which is exposed to the aerosol within the receiving cavity 4. As a consequence, the number of photons at each wavelength reaching the first and second sensor 121, 122 could change, which in turn could reduce the measurement accuracy. To overcome this issue, lens 111 is configured as scattering lens having a scattering back lens surface 112. The scattering surface 112 is a non-smooth lens surface having random irregularities from a smooth lens surface. Due to the scattering surface 112, the scattering lens 111 scatters thermal radiation emitted by the target surface 33, 233 in all directions. Consequently, the first and second sensors 121, 122 receive substantially an equal number of photons in all wavelengths, even though a part of a surface of the optical system is blocked by particle or droplet deposits 300.
(23)
(24) In both embodiments according to
(25) To further optimize the optical radiative transfer, the optical material of the lenses, 111, 114, 115, 117 is transparent for wavelength in the infra-red spectrum. In both embodiments, injection molding plastics, such as COC, is used as lens material allowing for mass production.
(26) As can be further seen from
(27) In order to hinder or even prevent dust and aerosol deposits on the front lenses 111, 115, the front surfaces of these lenses comprise a hydrophobic coating 113. The hydrophobic coating 113 also facilitates an easy cleaning of the front lens 111, 115.