Apparatus for Limiting a Time Integration Value of a Pulsed Current

1. Field of the Invention

This invention relates to an improvement of an electronic device in which a pulse current flows in a circuit element such as a LED (light emitting diode) or thermistor.

2. Prior Art

One example of a conventional electronic device of this type is a pulse oximeter. The pulse oximeter generally uses an LED. In order to increase the quantity of light of the LED, it is essential to increase the current flowing therein. However, the steady application of large current to the LED suffers from the following difficulties: Heat generated by the LED, (1) lowers the efficiency of the LED itself, (2) thermally damages the LED, and (3) damages vital tissues adjacent to the LED. Accordingly, when a large current is applied to the LED, it should be in the form of a pulse. However, it should be noted that, if the circuit is modified so as to apply a large current, in the form of a pulse to an LED, which becomes out of order (i.e., allows a large current to continuously flow in the LED), then the circuit will suffer from the same difficulties.

As was described above, when the conventional pulse oximeter becomes out of order to cause current, to continuously flow in the LED, the latter is overheated. However, the conventional pulse oximeter has no means for eliminating or preventing this difficulty. Only the pulse oximeter with the LED has been described; however, the preceding description is applicable to electronic devices having a circuit element which is driven by a pulse current and which should be prevented from being overheated.

Accordingly, an object of the invention is to provide an electronic device with a circuit element to which a pulse current is applied, in which the circuit element is prevented from being overheated.

The foregoing object and other objects of the invention have been achieved by the provision of an electronic device in which a pulse current flows in a circuit element, which according to the invention, comprises: means for limiting the time integration value of current flowing in the circuit element, the means being connected in series to the circuit element.

The nature, principle and utility of the invention will become more apparent from the following detailed description and the appended claims when read in conjunction with the accompanying drawings.

In the accompanying drawings:

FIG. 1 is a circuit diagram showing a first embodiment of the invention;

FIG. 2 is a circuit diagram showing an equivalent circuit of the circuit of FIG. 1 which is placed in a certain state;

FIGS. 3 and 4 are time charts for a description of the operation of the circuit shown in FIG. 1; and

FIG. 5 is a circuit diagram showing another embodiment of this invention.

Preferred embodiments of this invention will be described with reference to the accompanying drawings.

FIG. 1 shows a circuit around an LED in a pulse oximeter according to the invention. In FIG. 1, reference numeral 1 designates the LED; 2, a transistor 3, an operational amplifier; 4, 5 and 6, resistors; and 7, a capacitor. The anode of the LED 1 is connected to one connecting point of the resistor 4 and the capacitor 7. A constant voltage +E (V) is applied to the other connecting point of the resistor 4 and the capacitor 7. The cathode of the LED 1 is connected to the collector of the transistor 2. The base of the transistor 2 is connected through the resistor 6 to the output terminal of the operational amplifier 3, and the emitter is connected to the inversion input terminal (-) of the operational amplifier 3 and to one terminal of the resistor 5, the other terminal of which is held at 0 volt. A drive signal voltage V.sub.in (t) is applied to the non-inversion input terminal (+) of the operational amplifier 3.

In the circuit thus organized, the parallel circuit of the resistor 4 and the capacitor 7 is a means for limiting the time integration value of current flowing in the LED 1.

The operation of the circuit shown in FIG. 1 will be described with reference to FIGS. 3 and 4. In this connection, the voltage drop across the parallel circuit of the resistor 4 and the capacitor 7 is represented by V.sub.c (t); the voltage drop in the forward direction of the LED 1, V.sub.d (t); the Current flowing in the LED 1, I.sub.d (t); the voltage at the connecting point of the emitter of the transistor 2 and the resistor 5, V.sub.1 (t); the voltage at the anode of the LED 1, V.sub.2 (t); the resistances of the resistors 4, 5 and 6, R1, R2 and R3, respectively; and the capacitance of the capacitor 7, C.

FIG. 3 shows relationships between V.sub.1 (t), V.sub.2 (t), I.sub.d (t) and V.sub.d (t) in the case where the drive signal V.sub.in (t) is normal (i.e., not out of order). As is apparent from FIG. 3, in the case where the drive signal V.sub.ni (t) is a pulse wave V.sub.io in peak value, T.sub.d in pulse width and T.sub.t in period, the voltage V.sub. (t) changes with charge and discharge of the capacitor 7; however, the current I.sub.d (t) flowing in the LED 2 is a pulse wave synchronous with the pulse wave V.sub.ni (t), not depending on the value V.sub.2 (t). The peak value Ido of the current I.sub.d (t) is V.sub.in /R.sub.2.

FIG. 4 shows relationships between V.sub.1 (t), V.sub.2 (t), I.sub.d (t) and V.sub.d (t) in the case where the drive signal V.sub.ni (t) is abnormal (i.e., out of order), thus being held at V.sub.io for more than a predetermined period of time T.sub.s. The voltage V.sub.2 (t) becomes equal to (V.sub.1 (t)=Vdo) when the drive signal voltage V.sub.ni (t) reaches V.sub.io, for a period of time T.sub.s. In this case, the difference between the base voltage and the collector voltage of the transistor 2 becomes zero, and the transistor 2 is saturated, thus losing its current amplifying function. From this time instant, (i.e., from the time V.sub.in (t) reaches Vio for a period of time T.sub.s) the current I.sub.d (t) flowing in the LED 1 decreases, and after the lapse of a predetermined period of time the circuit of FIG. 1 becomes equivalent to that shown in FIG. 2. That is, the current I.sub.d (t) is held stable with I.sub.ds .congruent.E/R.sub.1. The circuit of FIG. 1 is so designated that V.sub.io /R.sub.2 >E/R.sub.1 is established. Therefore, even if the drive signal V.sub.ni (t) becomes abnormal or out of order as described above, the predetermined period of time after it is raised to V.sub.io the current I.sub.d (t) is maintained at a substantially small value E/R.sub.1, and therefore the LED 1 will never be overheated.

As is apparent from the above description, the embodiment of the invention is formed by adding the passive circuit element to the original drive circuit for driving a predetermined circuit element, and therefore it scarcely becomes out of order. That is, the electronic device provided by the invention is high in reliability.

One example of the medical instruments to which the technical concept of the invention is applicable is a thermistor thermometer.

The thermistor thermometer is used not only to measure a body temperature, but also to detect the number of respirations per unitary time. In the latter case, the thermistor thermometer is inserted into the nostril, so that the temperature difference between inhalation and exhalation. The operating principle of the thermistor thermometor is that current is applied to the thermistor so that the resistance of the thermistor which changes with temperature is detected as a variation in voltage. The sensitivity of measurement can be improved by increasing the amount of current applied to the thermistor; however, the method is disadvantageous in that the current thus increased raises the temperature of the thermistor element, resulting in an error in measurement. In order to eliminate this difficulty, a thermistor thermometer in which a pulse current is utilized to drive the thermistor element has been proposed. The technical concept of this invention may be applied to the thermistor thermometer thus proposed. That is, in this case, the means for limiting the time integration value of current is connected in series to the thermistor element therein. Therefore, even when the pulse current generating circuit or the like becomes out of order to allow the application of excessively large current, the trouble that the thermistor element is broken or the patient gets burned will never take place.

FIG. 5 shows one example of a circuit in which the thermistor thermometer is employed as a respiration monitor. In FIG. 5, reference numeral 10 designates a thermistor; 11, an amplifier for detecting and amplifying a voltage developed across the thermistor 10; 12, a rectifier circuit for rectifying the output of the amplifier 11; and 13, a meter for indicating the output value of the rectifier circuit 12. The other circuit elements are the same as those in FIG. 1, being designated by the same reference numerals. In FIG. 5, the parallel circuit of the resistor 4 and the capacitor 7 is the means for limiting the time integration value of current flowing in the thermistor 10. Even when, in the circuit thus organized, the drive signal becomes abnormal. The thermistor 10 will never be overheated.

As was described above, when an abnormal drive signal is applied to the device to allow current to flow in the circuit element for more than the predetermined period of time to which a pulse current is normally applied, the current is limited according to the invention so that the circuit element is prevented from being overheated. Accordingly, the device is prevented from damage, and can be applied to the living body with higher security.