Measuring arrangement for measuring an effective value of an AC voltage in a handheld power tool

Abstract

A hand-held power tool is disclosed with a measuring system for determining an effective value of an alternating voltage which is fed via an external conductor with respect to a neutral conductor. A regulated direct voltage source has a power supply potential which is referenced to the neutral conductor. There is a first resistance value from the power supply potential to a tap and a second resistance value from the tap to a ground. A voltmeter has a measurement range and its measurement input is connected to the tap. A measurement line connects the tap to the external conductor. The first resistance value is lower than the second resistance value such that the mean voltage value on the tap is equal to the mean of the measurement range for one period of the alternating voltage.

Claims

1. A hand-held power tool having a measuring system for determining an effective value of an alternating voltage supplied via an external conductor with respect to a neutral conductor, comprising: a regulated direct voltage source; a voltmeter which is supplied with power by the direct voltage source; a voltage divider disposed between a power supply potential and a ground and which has a first resistor between the power supply potential and a tap and a second resistor between the tap and the ground; wherein the voltmeter has a measurement range whose measurement input is connected to the tap and determines an effective voltage from a voltage on the tap; and a measurement line which connects the tap to the external conductor; wherein a first resistance value of the first resistor is lower than a second resistance value of the second resistor such that an average voltage value at the tap is equal to a mean of the measurement range for a period of the alternating voltage.

2. The hand-held power tool according to claim 1, wherein the following equation holds: R1/R2=(1−Vcc/Max), where R1 is the first resistance value, R2 is the second resistance value, Vcc is the power supply potential and Max is an upper limit voltage of the measurement range.

3. The hand-held power tool according to claim 1, wherein the measurement line includes a series resistor.

4. The hand-held power tool according to claim 1, further comprising an electric motor supplied with the alternating voltage.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

(1) FIG. 1: an illustration of a measurement of the voltmeter;

(2) FIG. 2: a schematic block diagram of one embodiment of a measuring system for measuring an effective value of an AC voltage in a hand-held power tool;

(3) FIG. 3: a measurement result of one embodiment of measuring an effective value of an AC voltage in a hand-held power tool; and

(4) FIG. 4: a schematic block diagram of one embodiment of a hand-held power tool.

DETAILED DESCRIPTION OF THE DRAWINGS

(5) The same elements or those having the same function are indicated by use of the same reference numerals in the figures, unless otherwise indicated.

(6) FIG. 2 shows a schematic block diagram of one embodiment of a measuring system 5 for measuring the effective value E of the alternating voltage U in a hand-held power tool.

(7) This shows the neutral conductor N and an exterior conductor L of a three-phase current feed. A power supply 24 carries the current to the internal consumer of the hand-held power tool, for example a motor. A DC voltage regulator 25 supplies a direct voltage range. The direct voltage regulator 25 taps the alternating voltage and converts the alternating voltage U1 into a fixed regulated direct voltage Vcc. The direct voltage regulator 25 references its potential to the voltage U1 of the neutral conductor L. The direct voltage regulator 25 pulls a ground 23 to a corresponding potential. The ground 23 is decoupled with respect to the potential Um of the external conductor L.

(8) A voltmeter 26 is supplied with power by the direct voltage Vcc of the direct voltage regulator 25. The voltmeter 26 utilizes the ground 23 as reference potential. The voltmeter 26 has a predefined measurement range, which is between ground 23 and the power supply voltage Vcc due to the power supply. The design of the voltmeter 26 can further restrict the measurement range and its resolution. As shown in FIG. 1, the measurement range Mb is limited at the top by the voltage max and at the bottom by the voltage min. The mean value MwMb of the measurement range Mb is the arithmetic mean of min and max. The measurement input of the voltmeter 26 is indirectly connected to the external conductor L. A measuring system 5 between the external conductor L and the A/D converter ensures an adaptation of the voltage level to maximally utilize the measurement range of the A/D converter 26.

(9) Measuring system 5 also comprises a series resistor R.sub.v and a voltage divider comprised of a first ohmic resistor 21 and a second ohmic resistor 22 with unequal resistance values R.sub.1, R.sub.2. The voltage divider 21, 22 is of dimensions such that the mean value Mw.sub.E of the alternating voltage U to be measured corresponds to the mean value Mw.sub.Mb of the measurement range Mb.

(10) The voltmeter 26 records the voltage Uout at the tap 27 for at least one period of the alternating voltage. The effective voltage can be calculated by integration (quadrature) of the recorded voltage Uout or with the assumed sinusoidal voltage calculated from the peak value of the voltage Uout. The voltmeter 26 may contain an A/D converter and optionally an integrator.

(11) FIG. 3 shows a measurement result of measurement of the effective value E of the alternating voltage U in a hand-held power tool according to the embodiment shown in FIG. 2. Due to the dimensioning of the voltage divider 21, 22 shown above, the mean value Mw.sub.E of the effective value E of the alternating voltage U to be measured corresponds to the mean value Mw.sub.Mb of the measurement range Mb, which thus prevents an offset between the mean value Mw.sub.E of the effective value E of the alternating voltage U to be measured and the mean value Mw.sub.Mb of the measurement range Mb, as shown in FIG. 1. The measurement range Mb is utilized optimally in this way.

(12) The calculation of the dimensioning of the voltage divider 21, 22 is shown below. Um is the alternating voltage potential on the external conductor L, Rv is the resistance value of the series resistor Rv, Uout is the potential at the measurement tap 27 of the voltage divider 21, 22.

(13) The following expression can be derived from Kirchoffs first law:

(14) $\begin{array}{cc}\frac{U_m-U_{\mathrm{out}}}{R_V}+\frac{V_{\mathrm{CC}}-U_{\mathrm{out}}}{R_1}=\frac{U_{\mathrm{out}}}{R_2}& \left(1\right)\end{array}$

(15) The measuring system is designed for a maximum peak voltage .Math., which is represented as the Max of the measurement range Mb:
U.sub.out=V.sub.CC;U.sub.m=U.sub.1+.Math.

(16) When inserted into equation (1), this yields

(17) $\begin{array}{cc}{R}_2=\frac{V_{\mathrm{CC}}}{\hat{U}+U_1-V_{\mathrm{CC}}}.Math.R_V& \left(2\right)\end{array}$

(18) At the maximum measurable negative peak voltage .Math., which represents the least of the value Min that can be displayed by the voltmeter, it holds that:
U.sub.out=0V;U.sub.m=U.sub.1−.Math.

(19) Again, when inserted into equation (1), it then follows that:

(20) $\begin{array}{cc}{R}_1=\frac{V_{\mathrm{CC}}}{\hat{U}-U_1}.Math.R_V& \left(3\right)\end{array}$

(21) At the zero crossing, it holds that U.sub.m=U.sub.1 and it should hold that U.sub.out=½*Vcc.

(22) Two variants 1 and 2 of the method described above are shown below as examples.

(23) Variant 1:

(24) Desired measurement range±288V.sub.eff; .Math.=±407V.sub.peak

(25) Output voltage OF power supply: U.sub.1=7.3V

(26) Power supply A/D converter: Vcc=5.0V

(27) Series resistor Rv=204 kΩ

(28) R.sub.1=2.55 kΩ R2=2.49 kΩ

(29) Variant 2:

(30) In this simplified variant, the power supply directly supplies the power supply voltage of the A/D converter, which means that U.sub.1=Vcc.

(31) Thus the two equations (2) and (3) are simplified to:

(32) $\begin{array}{cc}{R}_2=\frac{V_{\mathrm{CC}}}{\hat{U}}.Math.R_V& \left(2^{\prime }\right)\\ R_1=\frac{V_{\mathrm{CC}}}{\hat{U}-V_{\mathrm{CC}}}.Math.R_V& \left(3^{\prime }\right)\end{array}$
Desired measurement range: ±264V.sub.eff=380V.sub.peak
Output voltage power supply: U.sub.1=5.0V
Power supply A/D converter: Vcc=5.0V
Series resistor Rv=204 kΩ R.sub.1=2.72 kΩ R2=2.68 kΩ

(33) FIG. 4 shows a schematic block diagram of a first exemplary embodiment of a hand-held power tool 1, for example a jackhammer.

(34) The hand-held power tool 1 comprises an electric motor 2 which drives a tool 3, for example by means of a gear, a striker mechanism 10, etc. In addition, the hand-held power tool 1 has a control unit 4 for controlling the electric motor 2. The control unit 4 controls for example a power supply of the electric motor 2 and thereby controls a torque and/or a rotational speed of the electric motor 2.

(35) A user starts operation of the hand-held power tool 1 by operating a button 9. The button 9 is preferably arranged on a handle 6 with which the user can hold and guide the hand-held power tool 1.

(36) A power cord 8 on the hand-held power tool 1 supplies power as an electric voltage to the control unit 4 and the electric motor 2 as a function of the operation of the button 9. The power cord 8 preferably has three potential carrying lines (external conductors L). The power cord 8 may contain a neutral conductor N or the neutral conductor N may be guided by a star connection within the hand-held power tool 1 to the control unit 4 and the measuring system 5.

(37) A measuring system 5 serves to measure an effective value of an alternating voltage in the hand-held power tool 1. In the exemplary embodiment of the hand-held power tool 1 shown in FIG. 4, the measuring system 5 is part of the control unit 4. However, the measuring system 5 may also be arranged differently in the hand-held power tool 1, for example, as a separate component outside of the control unit 4.