Method and apparatus for detecting bubbles in a liquid

Claim 2

In the method of detecting the presence of bubbles in a liquid by sensing the effect of absorption by the liquid of radiation directed therethrough, the improvement which markedly increases the differential between the amount of radiation transmitted along a radiation path through the liquid when a bubble is not present in the radiation path and a greater amount of radiation transmitted through a bubble in the liquid present in the radiation path, comprising directing along said radiation path radiation having wavelength greater than 1.0 micrometer, and detecting the radiation having a wavelength greater than 1.0 micrometer which has traversed said radiation path.

Claim 3

The improved method of claim 1 wherein the liquid is an aqueous liquid.

Claim 4

An improved method of claim 1 wherein the liquid is blood.

Claim 5

The improved method of claim 1 wherein the radiation directed along said radiation path is filtered to limit the detected radiation to that having a wavelength greater than 1.0 micrometer.

Claim 6

The improved method of claim 1 wherein at least some of the radiation directed along the radiation path has a wavelength of between about 1.0 and 2.5 micrometers, and the radiation detected is that having a wavelength of between about 1.0 and 2.5 micrometers.

Claim 7

The improved method of claim 1 wherein at least some of the radiation directed along the radiation path has a wavelength of between about 1.4 and 2.5 micrometers, and the radiation detected is that having a wavelength of between about 1.4 and 2.5 micrometers.

Claim 8

The improved method of claim 1 wherein at least some of the radiation directed along the radiation path has a wavelength of about 1.45 micrometers, and the radiation detected is that having a wavelength of about 1.45 micrometers.

Claim 9

The improved method of claim 1 wherein at least some of the radiation directed along the radiation path has a wavelength of about 1.92 micrometers, and the radiation detected is that having a wavelength of about 1.92 micrometers.

Claim 10

The improved method of claim 1 wherein the radiation is supplied by a lamp operated at a temperature of the order of 1500° K.

Claim 11

The improved method of claim 1 wherein the liquid is aqueous, the radiation is supplied by a lamp operated at a temperature of the order of 1500° K. the output of which includes radiation having a wavelength of between about 1.0 and 2.5 micrometers, and the radiation detected is that having a wavelength of between about 1.0 and 2.5 micrometers.

Claim 12

The improved method of claim 1 wherein the liquid is aqueous, the radiation is supplied by a lamp operated at a temperature of the order of 1500° K. the output of which includes radiation having a wavelength of about 1.92 micrometers, and the radiation detected is that having a wavelength of about 1.92 micrometers.

Claim 13

In apparatus for detecting the presence of bubbles in a liquid by sensing the effect of absorption by the liquid of radiation directed from a source thereof along a radiation path through the liquid and toward a radiation-responsive sensor, the improvement which markedly increases the differential between the signal response of the sensor when a bubble is not present in the radiation path and the higher signal response thereof when a bubble in the liquid is present in said path, wherein at least some of the radiation directed from the source along the radiation path has a wavelength greater than 1.0 micrometer, and the sensor is responsive to radiation having a wavelength greater than 1.0 micrometer.

Claim 14

In apparatus for detecting the presence of bubbles in a liquid by sensing the effect of absorption by the liquid of radiation directed from a source thereof along a radiation path through the liquid and toward a radiation-responsive sensor, the improvement which markedly increases the differential between the signal response of the sensor when a bubble is not present in the radiation path and the higher signal response thereof when a bubble in the liquid is present in said path, wherein at least some of the radiation directed from the source along the radiation path has a wavelength greater than 1.0 micrometer, and the sensor is responsive to radiation having a wavelength greater than 1.0 micrometer.

Claim 15

The improved apparatus of claim 12 wherein the radiation source is a lamp operated at a temperature of the order of 1500° K.

Claim 16

The improved apparatus of claim 2 wherein at least some of the radiation directed from the source thereof along the radiation path has a wavelength of between about 1.4 and about 2.5 micrometers, and the sensor is responsive to radiation having a wavelength of between about 1.4 and 2.5 micrometers.

Claim 17

The improved apparatus of claim 12 wherein at least some of the radiation directed from the source thereof along the radiation path has a wavelength of about 1.45 micrometers, and the sensor is responsive to radiation having a wavelength of about 1.45 micrometers.

Claim 18

The improved apparatus of claim 12 wherein at least some of the radiation directed from the source thereof along the radiation path has a wavelength of about 1.92 micrometers, and the sensor is responsive to radiation having a wavelength of about 1.92 micrometers.

Claim 19

The improved apparatus of claim 2 having filter means in the radiation path for limiting to wavelengths greater than 1.0 micrometer the radiation from the source which can reach the sensor.

Claim 20

The improved apparatus of claim 12 having filter means in the radiation path for limiting to wavelengths between about 1.4 and about 2.5 micrometers the radiation from the source which can reach the sensor.

Claim 21

The improved apparatus of claim 12 having filter means in the radiation path for limiting to a wavelength of about 1.45 micrometers the radiation from the source which can reach the sensor.

Claim 22

The improved apparatus of claim 12 having filter means in the radiation path for limiting to a wavelength of about 1.92 micrometers the radiation from the source which can reach the sensor.

Claim 23

The improved apparatus of claim 12 having filter means in the radiation path for limiting to wavelengths greater than 1.0 micrometer the radiation from the source which can reach the sensor, said sensor and filter means being substantially matched such that the sensor has peak responsivity at substantially the wavelength of radiation from said source permitted by the filter means to reach said sensor.

Claim 24

The improved apparatus of claim 12 having filter means in the radiation path for limiting to wavelengths of about 1.4 to about 2.5 micrometers the radiation which can reach the sensor, and said sensor is responsive to radiation having a wavelength of from about 1.2 to about 2.5 micrometers.

Claim 25

The improved apparatus of claim 12 having a narrow bandpass interference filter in the radiation path for limiting to wavelengths of about 1.92 the radiation which can reach the sensor, and said sensor is a lead sulfide thermal detector responsive to radiation of a wavelength of from about 1.2 to about 2.5 micrometers and having a peak responsivity to radiation of a wavelength of about 2.0 micrometers.

Claim 26

The improved apparatus of claim 12 having filter means in the radiation path between the liquid and the sensor for limiting to wavelengths greater than 1.0 micrometer the radiation which can reach the sensor.

Claim 27

The improved apparatus of claim 12 wherein the liquid is contained in a radiation transmissive tube, there is means for focusing the radiation from the source toward the bore of the tube, and there is radiation collection means for collecting radiation from the source which has passed through the tube bore and for directing such radiation toward the sensor.

Claim 28

The improved apparatus of claim 12 wherein the liquid is contained in a radiation transmissive tube, there is wide aperature radiation collection means for collecting radiation from the source which has passed through the tube bore and for directing such radiation toward the sensor, and positioned between the collection means and the sensor is filter means for limiting to wavelengths greater than 1.0 micrometer the radiation which can reach the sensor.

Claim 29

The improved apparatus of claim 12 wherein the liquid is contained in a radiation transmissive tube, there is wide aperture fiber optic radiation collection means for collecting radiation from the source which has passed through the tube bore and for directing such radiation toward the sensor, and positioned between the collection means and the sensor is filter means for limiting to wavelengths greater than 1.0 micrometer the radiation which can reach the sensor.

Claim 30

The improved apparatus of claim 12 wherein the liquid is contained in a radiation transmissive tube; the radiation source is a lamp operated at a temperature of the order of 1500° K.; there is means for focusing the radiation from the lamp toward the bore of the tube; there is wide aperature radiation collection means for collecting radiation from the source which has passed through the tube bore and for directing such radiation toward the sensor; there is positioned between the collection means and the sensor a narrow bandpass interference filter which limits radiation which can reach the sensor to that having a wavelength of about 1.92 micrometers; and the sensor is a lead sulfide thermal detector responsive to radiation of a wavelength of from about 1.2 to about 2.5 micrometers and having a peak responsivity to wavelengths of about 2.0 micrometers.