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CN1012845B - thermal analysis device - Google Patents

thermal analysis device Download PDF

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CN1012845B
CN1012845B CN 86108245 CN86108245A CN1012845B CN 1012845 B CN1012845 B CN 1012845B CN 86108245 CN86108245 CN 86108245 CN 86108245 A CN86108245 A CN 86108245A CN 1012845 B CN1012845 B CN 1012845B
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voltage
sample
temperature
output
detection device
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CN86108245A (en
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松本慎吾
内池光正
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Shimadzu Corp
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Abstract

一种输出端具有补偿装置的热分析装置。设有输出随检测装置输出的样品温度电压而变化的非线性电压的折线函数电压发生装置。与此同时还没有乘法装置,把折线函数电压同检测装置检测的温差电压相乘,或设有分压装置,以折线函数电压为控制电压产生一个与检测装置灵敏度特性对称的可变阻抗装置,对检测装置输出的温差电压进行分压。用本发明可补偿检测灵敏度的温度依赖性,使得能够正确地进行热分析。

A thermal analysis device having a compensation device at the output. There is a broken-line function voltage generating device that outputs a nonlinear voltage that changes with the sample temperature voltage output by the detection device. At the same time, there is no multiplication device, which multiplies the broken line function voltage with the temperature difference voltage detected by the detection device, or a voltage divider, which uses the broken line function voltage as the control voltage to generate a variable impedance device symmetrical to the sensitivity characteristics of the detection device. Divide the temperature difference voltage output by the detection device. The temperature dependence of detection sensitivity can be compensated with the present invention, enabling correct thermal analysis.

Description

本发明是关于在输出端备有补偿装置的热分析装置,补偿装置对检测装置检测灵敏度的温度依赖性进行补偿。The invention relates to a thermal analysis device provided at the output with compensating means for compensating the temperature dependence of the detection sensitivity of the detection means.

例如,对于高分子物质的状态变化的分析,大多使用热流型示差热量测定装置。在这种装置中,把插入样品的样品容器和插入标准物质的标准容器放在置于加热炉内的传热板上,以一定的升温速度使之加热,在此过程中发生的样品吸热和发热现象所引起的热能的传递和接收通过传热板进行,与此同时,对由两个热电偶构成的检测装置检测到的示差热量进行测定。For example, heat flow type differential calorimeters are often used for analysis of state changes of polymer substances. In this device, the sample container inserted into the sample and the standard container inserted into the standard substance are placed on a heat transfer plate placed in a heating furnace, and heated at a certain rate of temperature rise, and the heat absorbed by the sample occurs during this process. The transmission and reception of heat energy caused by the heating phenomenon is carried out through the heat transfer plate, and at the same time, the differential heat detected by the detection device composed of two thermocouples is measured.

在这种装置中,由于传递和接收热能的传热板的热传导率随温度上升而变化,并且热传递还受到与周围温度相对应的辐射、对流等因素的影响,所以,两个热电偶构成的检测装置对样品的吸热和发热的检测灵敏度表现出随加热温度上升而降低的特性。因此,表示样品吸热和发热的峰值波形的振幅就随加热温度的上升而减小。因此,尽管采取了在加热炉的上、下面复盖有光泽的均热砖块以防止检测装置偏热,但是,既然是一边使加热炉的加热温度以一定速度上升,一边进行测定,就不可能与周围温度的变化无关,所以,输出峰值波形的振幅随温度而变化的问题依然存在。In this device, since the thermal conductivity of the heat transfer plate that transmits and receives heat energy changes as the temperature rises, and the heat transfer is also affected by factors such as radiation and convection corresponding to the ambient temperature, the two thermocouples constitute The detection sensitivity of the detection device to the heat absorption and heat generation of the sample shows a characteristic that decreases with the increase of the heating temperature. Therefore, the amplitude of the peak waveform representing the heat absorption and heat generation of the sample decreases as the heating temperature increases. Therefore, although the heating furnace is covered with glossy soaking bricks to prevent the detection device from being overheated, since the heating temperature of the heating furnace is raised at a certain speed while the measurement is performed, it is not Probably not related to changes in ambient temperature, so the problem of the amplitude of the output peak waveform changing with temperature still exists.

鉴于上述问题,本发明的目的是提供一种经过改进的热分析装置,在检测装置的输出端对其检测灵敏度进行补偿,使之不受周围温度的影响。In view of the above problems, it is an object of the present invention to provide an improved thermal analysis device whose detection sensitivity is compensated at the output of the detection device so that it is not affected by the ambient temperature.

也就是说,本发明的特征是:设有检测装置和折线函数电压发生装置,检测装置将表示热量检测灵敏度随加热炉加热温度上升而降低特性的标准物质同样品的温差及样品温度分别输出,折线函数电压发生装置输出随上述检测装置输出的样品温度电压的增加而变化的非线性电压,与此同时,还具有乘法运算装置或分压装置,乘法运算装置把上述折线函数电压发生装置发生的电压同上述检测装置检测的标准物质与样品的温差电压进行乘法运算,分压装置以上述折线函数电压发生装置发生的电压为控制电压,通过其内阻可随上述控制电压振幅变化,变换为具有与上述检测装置检测灵敏度特性对称特性的可变阻抗装置,对上述检测装置输出的标准物质与样品的温差电压进行分压。That is to say, the feature of the present invention is: be provided with detecting device and broken-line function voltage generating device, detecting device will show that the temperature difference and sample temperature of the standard substance that the heat detection sensitivity of heating furnace heating temperature rises and reduce characteristic and sample temperature respectively, The broken-line function voltage generating device outputs a nonlinear voltage that changes with the increase of the sample temperature voltage output by the above-mentioned detection device. At the same time, it also has a multiplication device or a voltage divider. The voltage is multiplied with the temperature difference voltage of the standard substance detected by the above-mentioned detection device and the sample. The voltage divider uses the voltage generated by the above-mentioned broken-line function voltage generator as the control voltage, and its internal resistance can change with the amplitude of the above-mentioned control voltage. The variable impedance device, which is symmetrical to the detection sensitivity characteristic of the detection device, divides the temperature difference voltage between the standard substance and the sample output by the detection device.

在把热量检测灵敏度随加热炉的加热温度的增加而降低的检测装置检测的标准物质与样品的温差电压输给乘法运算装置的同时,把电压增加率随检测装置检测的样品温度电压的上升而变化的非线性电压为补偿电压,也输给乘法运算装置,通过将补偿电压同标准物质与样品的温差电压进行乘法运算,对标准物质与样品温差电压峰值面积的减小进行补偿。While the thermal detection sensitivity decreases with the increase of the heating temperature of the heating furnace, the temperature difference voltage between the standard substance and the sample detected by the detection device is output to the multiplication device, and the voltage increase rate is increased with the temperature and voltage of the sample detected by the detection device. The changing nonlinear voltage is the compensation voltage, which is also output to the multiplication device. By multiplying the compensation voltage with the temperature difference voltage between the standard substance and the sample, the reduction of the peak area of the temperature difference voltage between the standard substance and the sample is compensated.

另外,以上述非线性电压为控制电压输给可变阻抗装置的控制极,通过该控制电压,使可变阻抗装置的内阻获得与检测装置检测灵敏度对称的特性,从而输出经过补偿的不受检测装置热量检测灵敏度影响的标准物质与样品的温差电压。In addition, the above-mentioned non-linear voltage is used as the control voltage to output to the control electrode of the variable impedance device, and through the control voltage, the internal resistance of the variable impedance device obtains a characteristic that is symmetrical to the detection sensitivity of the detection device, thereby outputting the compensated The temperature difference voltage between the standard substance and the sample affected by the thermal detection sensitivity of the detection device.

第1图是本发明的一个实施例的结构图,第2图(A)是热电偶的热量检测灵敏度特性曲线图和吸热与发热的峰值波形图,第2图(B)是折线函数电压发生器的输出电压波形图。Figure 1 is a structural diagram of an embodiment of the present invention, Figure 2 (A) is a heat detection sensitivity characteristic curve of a thermocouple and peak waveforms of heat absorption and heat generation, and Figure 2 (B) is a broken line function voltage Generator output voltage waveform diagram.

第3图是本发明的另一实施例装置的结构图,第4图(A)是热 电偶的吸热与发热的热量检测灵敏度特性曲线和经场效应晶体管补偿后的内阻特性曲线图,第4图(B)是未经场效应晶体管补偿过的内阻特性曲线图和折线函数电压发生器的输出电压波形图。在图中:Fig. 3 is a structural diagram of another embodiment device of the present invention, and Fig. 4 (A) is a thermal The heat detection sensitivity characteristic curve of the heat absorption and heat generation of the galvanic couple and the internal resistance characteristic curve after compensation by the field effect transistor. Figure 4 (B) is the internal resistance characteristic curve and the broken line function without compensation by the field effect transistor The output voltage waveform diagram of the voltage generator. In the picture:

1……加热炉1...Heating furnace

5、5′……热电偶5, 5'... thermocouple

10、8、9……折线函数电压发生器10, 8, 9... Broken-line function voltage generator

12……乘法运算器12...Multiplier

15……场效应晶体管15...field effect transistor

下面,根据附图所示的实施例对本发明作详细说明。Hereinafter, the present invention will be described in detail according to the embodiments shown in the drawings.

附图表示的都是本发明的实施例,第1图中的符号1是加热炉,其中装有用铜等材料制成的传热板2,插入样品的样品容器3和插入标准物质的标准容器4放在该传热板2上,同时,该传热板2上还装有用来检测样品温度及标准物质温度并将样品温度和标准物质与样品的温差分别输出的热电偶5和5′,如图2(A)的特性曲线a所示,热电偶5和5′的热量检测灵敏度随加热温度的上升而降低。另外,在第2图(A)中,以实线表示的标准物质与样品的温差电压在样品吸热和发热过程中的峰值波形C,这是受热量检测灵敏度影响而峰值面积减小的补偿之前的波形,以虚线表示的是经过补偿后的峰值波形。6和7是放大器,分别用来放大热电偶5和5′检测的标准物质与样品的温差电压和热电偶5′检测的样品温度电压,放大器6与乘法运算器12的X端连接,放大器7与折线函数电压发生器8~10相接。折线函数电压发生器8~10的结构为:电阻R1~R3、R4~R6和R7~R9组成的三个串联电路相互并联,同时,在反馈环和输出端分别接有二极管D、D。电阻R2、R5和R8的一端分别连接在运算放大器OP1、OP2和OP3的输入端,它们的另一端分别通过二极管D与各自运算放大器的输出端相连。各运算放大器采用反相 输入方式,正端接地,并且,把大小各不相同的偏压加到运算放大器OP1~OP3的反相输入端,各个偏压取自由四个电阻组成的串联电路,该串联电路的两端分别外加+15V和-15V的电压。折线函数电压发生器8~10随着放大器7的输出电压增大,首先通过把上述各个串联电路并联起来的电阻回路,然后顺序使与运算放大器OP1、OP2和OP3连接的二极管D、D导通,输出第2图(B)所示的按对数式压缩的折线函数电压曲线b,并通过放大器11输给乘法运算器12的Y端,经过乘法运算的电压通过Z端输给图中未示出的数据处理装置。另外,这些电压发生器8~10可以输出具有倾斜特性的非线性电压,对标准物质与样品的温差所影响的热量检测灵敏度特性进行补偿。What accompanying drawing represents all is the embodiment of the present invention, and the symbol 1 among the 1st figure is a heating furnace, wherein the heat transfer plate 2 made of materials such as copper is housed, the sample container 3 that inserts sample and the standard container that inserts standard substance 4 placed on the heat transfer plate 2, meanwhile, the heat transfer plate 2 is also equipped with thermocouples 5 and 5′ for detecting the temperature of the sample and the temperature of the standard substance and outputting the temperature difference between the sample temperature and the standard substance and the sample respectively, As shown in the characteristic curve a of Fig. 2(A), the heat detection sensitivity of the thermocouples 5 and 5' decreases as the heating temperature rises. In addition, in Figure 2 (A), the peak waveform C of the temperature difference voltage between the standard substance and the sample represented by the solid line during the heat absorption and heat generation process of the sample is the compensation for the reduction of the peak area due to the influence of the heat detection sensitivity For the previous waveform, the dashed line represents the peak waveform after compensation. 6 and 7 are amplifiers, which are respectively used to amplify the temperature difference voltage between the standard substance and the sample detected by thermocouple 5 and 5′ and the temperature voltage of the sample detected by thermocouple 5′. Amplifier 6 is connected to the X terminal of multiplier 12, and amplifier 7 It is connected with the broken line function voltage generators 8-10. The structure of the broken-line function voltage generators 8-10 is: three series circuits composed of resistors R 1 -R 3 , R 4 -R 6 and R 7 -R 9 are connected in parallel with each other, and at the same time, the feedback loop and the output end are respectively connected with Diodes D, D. One ends of the resistors R 2 , R 5 and R 8 are respectively connected to the input ends of the operational amplifiers OP 1 , OP 2 and OP 3 , and their other ends are respectively connected to the output ends of the respective operational amplifiers through diodes D. Each operational amplifier adopts the inverting input mode, the positive terminal is grounded, and the bias voltages of different sizes are added to the inverting input terminals of the operational amplifiers OP 1 ~ OP 3 , and each bias voltage is taken from a series circuit composed of four resistors , The voltages of +15V and -15V are respectively applied to the two ends of the series circuit. As the output voltage of the amplifier 7 increases, the broken-line function voltage generators 8-10 firstly pass through the resistance loop that connects the above-mentioned series circuits in parallel, and then sequentially make the diodes D , D , and D is turned on, output the logarithmically compressed broken line function voltage curve b shown in Figure 2 (B), and output it to the Y terminal of the multiplier 12 through the amplifier 11, and the multiplied voltage is output to the figure through the Z terminal not shown in the data processing device. In addition, these voltage generators 8-10 can output non-linear voltages with slope characteristics to compensate the heat detection sensitivity characteristics affected by the temperature difference between the standard substance and the sample.

在这样构成的装置中,如果使加热炉1的加热温度上升,则可相应地通过放大器6把第2图(A)中实线表示的热电偶5和5′检测的峰面积减小后的峰值波形C的示差热温度电压输给乘法运算器12的X端。另一方面,通过放大器7把热电偶5检测的增大的样品温度电压输给折线函数电压发生器8~10。由此,在放大器7的输出电压达到V1之前,电流便经过电阻R1~R3、R4~R6和R7~R9组成的并联电路进行分流,输出第2图(B)的特性曲线b所示的线性电压,在该电压从V1变到V2期间,运算放大器OP1的二极管D、D导通,形成与电阻R2并联的电路,从而使合电阻减小,输出电压增加率降低;其次,在电压从V2变到V3期间,运算放大器OP2的二极管D、D导通,形成与电阻R5并联的电路,合电阻进一步减小,于是,输出电压增加率进一步地降低;最后,在电压从V3变到V4期间,运算放大器OP3的二极管D、D导通,形成与电阻R8并联的电路,输出电压增加率更进一步地减小。以折线函数 电压发生器8~10的对数式压缩电压为补偿电压,通过放大器11输给乘法运算器12的Y端。由于折线函数电压发生器8~10输出的补偿电压随样品温度电压的上升而增加,所以,在乘法运算器12中,每当输入以实线表示的示差热温度的振幅减小的峰值波形C时,就把这时的补偿电压值作为系数与该峰值波形C的振幅值进行乘法运算,由此将振幅减小的峰值波形C补偿为虚线表示的振幅增大的波形然后,通过正端输出。In the device constructed in this way, if the heating temperature of the heating furnace 1 is increased, the peak areas detected by the thermocouples 5 and 5' indicated by the solid lines in Fig. 2 (A) can be correspondingly reduced by the amplifier 6. The differential thermal temperature voltage of the peak waveform C is output to the X terminal of the multiplier 12 . On the other hand, the increased sample temperature voltage detected by the thermocouple 5 is output to the broken-line function voltage generators 8-10 through the amplifier 7. Thus, before the output voltage of the amplifier 7 reaches V1 , the current is shunted through the parallel circuit composed of resistors R1 - R3 , R4 - R6 and R7 - R9 , and the output voltage of Figure 2 (B) is The linear voltage shown in the characteristic curve b, during the period when the voltage changes from V 1 to V 2 , the diodes D and D of the operational amplifier OP 1 are turned on to form a circuit connected in parallel with the resistor R 2 , so that the combined resistance decreases and the output The voltage increase rate decreases; secondly, during the voltage change from V2 to V3 , the diodes D and D of the operational amplifier OP2 are turned on to form a circuit connected in parallel with the resistor R5 , and the combined resistance is further reduced, so the output voltage increases The rate is further reduced; finally, during the voltage change from V3 to V4 , the diodes D and D of the operational amplifier OP3 are turned on, forming a circuit connected in parallel with the resistor R8 , and the output voltage increase rate is further reduced. The logarithmic compressed voltage of the broken-line function voltage generators 8-10 is used as the compensation voltage, which is output to the Y terminal of the multiplier 12 through the amplifier 11 . Since the compensation voltage output by the broken-line function voltage generators 8-10 increases with the rise of the sample temperature voltage, in the multiplier 12, whenever the amplitude of the differential thermal temperature represented by the solid line is input, the peak waveform C At this time, the compensation voltage value at this time is used as a coefficient to multiply the amplitude value of the peak waveform C, thereby compensating the peak waveform C with a reduced amplitude to a waveform with an increased amplitude indicated by a dotted line, and then outputting it through the positive terminal .

下面,说明本发明的另外一个实施例。Next, another embodiment of the present invention will be described.

第3图是本发明的另外一个实施例的装置,和第1图相同的部分所标符号相同。Fig. 3 is a device of another embodiment of the present invention, and the same parts as Fig. 1 are marked with the same symbols.

在本实施例中,放大器6通过电阻R0与场效应晶体管(FET)15的源极连接,场效应晶体管15具有第4图(B)的特性曲线d所示的内阻随栅极电压0~Vn按线性地急剧增大的特性,折线函数电压发生器8~10通过放大器11与场效应晶体管15的栅极连接。另外,折线函数电压发生器8~9的结构考虑了检测部件的检测灵敏度特性和场效应晶体管15的栅偏压与内阻特性,因而,能够产生使检测部件的检测灵敏度与加热温度成线性关系的折线函数电压。In this embodiment, the amplifier 6 is connected to the source of the field effect transistor (FET) 15 through the resistor R 0 , and the field effect transistor 15 has the internal resistance shown in the characteristic curve d of Fig. ˜Vn increases rapidly linearly, and the broken line function voltage generators 8 ˜ 10 are connected to the gate of the field effect transistor 15 through the amplifier 11 . In addition, the structure of the broken-line function voltage generators 8-9 considers the detection sensitivity characteristics of the detection components and the gate bias and internal resistance characteristics of the field effect transistor 15, so that the detection sensitivity of the detection components can be linearly related to the heating temperature. The broken line function voltage.

13是放大器,它把放大器6的输出电压经电阻R0和场效应晶体管15分压后,将场效应晶体管15的分压输给图中未示出的数据处理装置。另外,图中的符号14是为了补偿场效应晶体管的特性偏差而加的调整电路,用来调整输给栅极的偏压。13 is an amplifier, which outputs the divided voltage of the field effect transistor 15 to a data processing device not shown in the figure after the output voltage of the amplifier 6 is divided by the resistor R0 and the field effect transistor 15. In addition, the symbol 14 in the figure is an adjustment circuit added to compensate the characteristic deviation of the field effect transistor, and is used to adjust the bias voltage output to the gate.

在这样构成的装置中,如果使加热炉1的加热温度上升,则相应地通过放大器6把热电偶5和5′检测的标准物质与样品的温差电压输给场效应晶体管15的源极。另一方面,通过放大器7把热电偶5检测的增大的样品温度电压输给折线函数电压发生器8~10。由 此,在放大器7的输出电压达到V1之前,电流便经电阻R1~R3、R4~R6和R7~R9组成的并联电路进行分流,输出第2图(B)的特性曲线b所示的线性电压,在该电压从V1变到V2期间,运算放大器OP1的二极管D、D导通,形成与电阻R2并联的回路,从而使合电阻减小,于是,输出电压增加率降低。其后,在电压从V2变到V3期间,运算放大器OP2的二极管D、D导通,形成与电阻R5并联的回路,合电阻进一步减小,于是,输出电压增加率进一步降低,最后,在电压从V3变到V4期间,运算放大器OP3的二极管D、D导通,形成与电阻R8并联的回路,输出电压增加率更进一步地减小。这样,由于折线函数电压发生器8~10是通过放大器11把电压振幅按对数式压缩成0~V4的电压后加到场效应晶体管15的栅极上的,所以,如第4图(B)的特性曲线e所示,与输入线性栅极电压0~Vn的情况相比,场效应晶体管其电压范围减小为0~V4,同时,该范围内的内阻增加率也受上述特性曲线e所表示的按对数式压缩后的电压控制,于是,检测灵敏度特性曲线就补偿为与第2图(A)中的a对称的第4图(A)所示的特性曲线α′。In the device constructed in this way, if the heating temperature of the heating furnace 1 is increased, the temperature difference voltage between the standard substance and the sample detected by the thermocouples 5 and 5 ′ is output to the source of the field effect transistor 15 through the amplifier 6 accordingly. On the other hand, the increased sample temperature voltage detected by the thermocouple 5 is output to the broken-line function voltage generators 8-10 through the amplifier 7. Thus, before the output voltage of the amplifier 7 reaches V1 , the current is shunted through the parallel circuit composed of resistors R1 ~ R3 , R4 ~ R6 and R7 ~ R9 , and outputs the For the linear voltage shown in the characteristic curve b, during the period when the voltage changes from V 1 to V 2 , the diodes D and D of the operational amplifier OP 1 are turned on to form a loop connected in parallel with the resistor R 2 , thereby reducing the combined resistance, so , the output voltage increase rate decreases. Thereafter, during the period when the voltage changes from V2 to V3 , the diodes D and D of the operational amplifier OP2 are turned on, forming a loop connected in parallel with the resistor R5 , and the combined resistance is further reduced, so the output voltage increase rate is further reduced, Finally, during the period when the voltage changes from V3 to V4 , the diodes D and D of the operational amplifier OP3 are turned on, forming a loop connected in parallel with the resistor R8 , and the output voltage increase rate is further reduced. In this way, since the broken-line function voltage generators 8-10 compress the voltage amplitude logarithmically into a voltage of 0- V4 through the amplifier 11 and then add it to the gate of the field effect transistor 15, so, as shown in Figure 4 (B) As shown in the characteristic curve e of the field effect transistor, compared with the case where the input linear gate voltage is 0-Vn, the voltage range of the field effect transistor is reduced to 0-V 4 , and at the same time, the internal resistance increase rate in this range is also affected by the above-mentioned characteristic curve The voltage control after logarithmic compression represented by e, so the detection sensitivity characteristic curve is compensated to the characteristic curve α' shown in Fig. 4 (A) which is symmetrical to a in Fig. 2 (A).

因此,如果把伴随放大器6输出的样品的吸热和发热的峰值功率输给场效应晶体管15,则该峰值电流与经过补偿的内阻进行乘法运算后的分压便输给放大器13,由于该分压随着加热温度的上升而增加,所以,随加热温度的上升而减小的峰值功率就可以得到补偿。Therefore, if the peak power of the heat absorption and heat generation of the sample output with the amplifier 6 is output to the field effect transistor 15, the divided voltage after the multiplication of the peak current and the compensated internal resistance is output to the amplifier 13, because the The partial pressure increases with increasing heating temperature, so the decrease in peak power with increasing heating temperature can be compensated.

另外,虽然在本实施例中说明的是把检测部件的检测灵敏度补偿装置应用于示差扫描热量测定装置中的情况,但是,这种补偿装置也可以应用于示差热分析装置,并且,折线函数电压发生器的数量可以根据对折线电压所希望的倾斜度的要求适当增减。此外,虽然在本实施例中折线函数电压发生器是按照电压增加率以对数式压缩而减小的 方式构成的,但是,通过改变二极管的连接方向,也可以做成使电压增加率增大的形式。In addition, although it is described in this embodiment that the detection sensitivity compensating device of the detection part is applied to the differential scanning calorimetry device, this compensating device can also be applied to the differential thermal analysis device, and the broken line function voltage The number of generators can be appropriately increased or decreased according to the desired slope of the broken-line voltage. In addition, although in this embodiment the broken line function voltage generator is reduced logarithmically in accordance with the voltage increase rate However, by changing the connection direction of the diode, it can also be made to increase the voltage increase rate.

如上所述,由于本发明是以折线函数电压发生装置输出的电压增加率发生变化的非线性电压为补偿电压与检测装置输出的标准物质与样品的温差电压进行乘法运算的,所以,即使检测装置的热量检测灵敏度随加热电流的增大而降低,并由此引起标准物质与样品的温差电压的振幅减小,也能够通过与上述补偿电压作乘法运算使标准物质与样品的温差电压的振幅增大,从而补偿其减小的部分,因此,能够输出换算成不受检测装置温度依赖性影响的标准物质与样品的温差电压,进行正确的热分析。As mentioned above, since the present invention multiplies the temperature difference voltage between the standard substance and the sample output by the detection device with the non-linear voltage whose output voltage increase rate of the broken-line function voltage generator changes as the compensation voltage, so even if the detection device The thermal detection sensitivity decreases with the increase of the heating current, and thus the amplitude of the temperature difference voltage between the standard substance and the sample decreases, and the amplitude of the temperature difference voltage between the standard substance and the sample can also be increased by multiplying the above-mentioned compensation voltage. Therefore, it is possible to output the temperature difference voltage between the standard substance and the sample, which is not affected by the temperature dependence of the detection device, and perform accurate thermal analysis.

另外,由于是把检测装置检测的样品温度电压输给折线函数电压发生装置,并把电压增加率随样品温度电压增加而减小的按对数式压缩后的非线性电压为控制电压输给可变阻抗装置的控制极,所以,加在可变阻抗装置的控制极上的控制电压范围缩小了,可以使该范围内的可变阻抗装置的内阻形成与上述检测装置的检测灵敏度特性对称的特性,因此,可以把表示样品的吸热和发热的峰值功率补偿为不受检测装置温度依赖性影响,从而能够进行正确的热分析。In addition, since the temperature and voltage of the sample detected by the detection device is input to the broken line function voltage generator, and the nonlinear voltage after logarithmic compression whose voltage increase rate decreases with the increase of the sample temperature and voltage is output as the control voltage to the variable The control pole of the impedance device, so the control voltage range applied to the control pole of the variable impedance device is narrowed, and the internal resistance of the variable impedance device within this range can be formed to be symmetrical with the detection sensitivity characteristics of the above-mentioned detection device , Therefore, the peak power indicating the heat absorption and heat generation of the sample can be compensated so as not to be affected by the temperature dependence of the detection device, thereby enabling accurate thermal analysis.

Claims (1)

1, a kind of apparatus for thermal analysis is characterized in that comprising: pick-up unit, the heat detection sensitivity is exported to a multiplying device respectively with the rise standard substance that reduces and the temperature difference and the sample temperature of sample of the heating-up temperature of heating furnace; The polygronal function device for generating voltage, the non-linear voltage that will change with the increase of the sample temperature voltage of above-mentioned detection device output is also exported to described multiplying device; Multiplying device or bleeder mechanism, described multiplying device carries out multiplying to the voltage that above-mentioned polygronal function device for generating voltage produces with the standard substance of above-mentioned detection device detection and the thermoelectric voltage of sample, the voltage that bleeder mechanism produces with above-mentioned broken line device for generating voltage is control voltage, by variable impedance apparatus the standard substance of above-mentioned detection device output and the thermoelectric voltage of sample are carried out dividing potential drop, the internal resistance of variable impedance apparatus can be transformed to the characteristic that has with the detection sensitivity characteristic symmetry of above-mentioned detection device with the amplitude of above-mentioned control voltage.
CN 86108245 1985-12-23 1986-12-22 thermal analysis device Expired CN1012845B (en)

Applications Claiming Priority (4)

Application Number Priority Date Filing Date Title
JP291004/85 1985-12-23
JP29100585A JPH0692947B2 (en) 1985-12-23 1985-12-23 Thermal analyzer
JP291005/85 1985-12-23
JP60291004A JP2581669B2 (en) 1985-12-23 1985-12-23 Thermal analyzer

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CN86108245A CN86108245A (en) 1987-07-01
CN1012845B true CN1012845B (en) 1991-06-12

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Publication number Priority date Publication date Assignee Title
WO2009074091A1 (en) * 2007-12-05 2009-06-18 Chery Automobile Co., Ltd. A motor torque smoothing treatment method for hybrid power and a hybrid power system

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EP1494126B1 (en) * 2003-07-04 2007-08-29 Mettler-Toledo AG Method and Apparatus for the examination of a material
EP2214005B1 (en) 2009-02-03 2019-09-18 Mettler-Toledo GmbH Thermo-Analytical Instrument

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2009074091A1 (en) * 2007-12-05 2009-06-18 Chery Automobile Co., Ltd. A motor torque smoothing treatment method for hybrid power and a hybrid power system

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