Isolated pH Monitor with Temperature Compensation


Knowing the pH value of a liquid is essential in many industries. Nearly every industry that handles liquids need a measurement system for pH. Obviously, it is important for waste water systems and waste water plants, but did you know that the water from a brewery needs to have a special pH value before it reaches the sewage water system? This design tip is intended to help adding high precision isolation to water treatment systems.

This article discusses the addition of high precision isolation to a system. This is essential for monitoring water pH that is located far from the system, monitoring differing ground levels, or for protecting a system from high voltage when an error occurs.

The pH value is a measure of the acidity or basicity of an aqueous solution. It is a unitless number and is defined as the negative common logarithm of the hydrogen ion activity according to the following equation:


Pure water is defined as having a pH value of 7, while acids have values of less than 7 and bases have values above 7. So-called indicators that change color according to the pH value are often used for measuring the pH. However, this measurement only provides a rough estimate. The circuit shown in Figure 1 is intended for evaluation of combined glass electrodes. It has an accuracy of 0.5% for the pH range from 0 to 14 and is temperature compensated. The circuit supports a large range of pH sensors, which can have high impedance values from 1 MΩ to a few GΩ.

Figure 1. pH sensor circuit with combined electrode (simplified).

The pH Electrode

The pH probe consists of a measuring electrode and a reference electrode, which is comparable to a battery. If the probe is dipped into a test solution, the measurement electrode generates a voltage depending on the hydrogen ion activity. A typical output value is 59.14 mV per unit of pH at 25°C. Due to the temperature dependency, this value can rise to 70 mV/pH. This voltage is compared with the reference electrode. If the test solution is acidic (low pH), the potential at the probe output is greater than 0; for a basic solution, it is less than 0. The output value can be calculated using the following equation:


E is the output voltage of the probe.
E0 is the standard electrode potential (typically 0 V), dependent on the probe.
R is the universal gas constant. R = 8.31447 J mol−1 K−1.
T is the temperature in Kelvin.
n is the number of transferred electrons (or equivalent number).
F is the Faraday constant. F = 96485.34 C mol−1.
pH is the hydrogen ion concentration of unknown solution.
pHREF = 7, reference value of reference electrode.

The Circuit

The three main elements of the circuit are the buffer for the probe, the ADC, and the isolator with the voltage transmission. The buffer op amp AD8603 was selected because it has low power consumption, low noise, and extremely low input bias current. The low input bias current of typically 200 fA ensures that the voltage drop due to current flow across the internal resistor of the probe is minimized. Another important component is the ADC, represented here by the AD7793, a 24-bit Σ-Δ converter with an integrated power source and programmable amplifier. The integrated current source generates the current that flows through the Pt1000. With this, the temperature measurement needed for compensation in the processor is performed. The same current also flows through the 5 kΩ resistor (0.1% tolerance), which thereby generates the reference voltage of 1.05 V. As a second function, the resistor boosts the common-mode voltage. Through this and through selection of the reference voltage, the input range of the ADC is fully utilized: the probe outputs ±414 mV—a maximum ±490 mV. The isolator is the ADuM5411, an isolated dc-to-dc converter that simultaneously provides for isolation of the SPI interface of the ADC.

Circuit Characteristics

To achieve high accuracy, the op amp was selected with a typical input bias current of 200 fA, which leads to a maximum voltage offset of 0.2 mV at the probe impedance of 1 GΩ. This corresponds to an error of 0.0037 units of pH at 25°C. Even with a maximum input bias current of 1 pA, the maximum offset error is very low, at 1 mV. In order not to give away this good starting position, it is advisable to take suitable layout measurements by using, for example, a guard ring, shielding, and other techniques that are not affected by very low currents. At the selected data rate of 16.7 Hz and a gain of 1, the noise generated by the ADC is approximately 2 µV rms. If the calculation is done with a peak-to-peak noise of 13 µV, the accuracy of the pH value is 0.00022 units of pH. If the noise from the amplifier and the noise from the ADC are taken together, this yields 0.00053 units of pH—and, hence, the offset error is much more significant.


The circuit shown here is a simple, very precise, and power-saving variant for pH sensor readings. Once the circuit has been calibrated, an accuracy of 0.5%, corresponding to 0.005 units of pH can be achieved. Thanks to the isolation, it is suitable for numerous applications.

Thomas Tzscheetzsch

Thomas Tzscheetzsch

Thomas Tzscheetzsch は、2010 年にシニア・フィールド・アプリケーション・エンジニアとしてアナログ・デバイセズに入社しました。2010 ~ 2012 年にドイツ中部地区の顧客を担当した後、より小規模な顧客層を対象とするキー・アカウント・チームに所属していました。2017 年の組織再編後は、FAE マネージャとして CE諸国の IHC クラスタにおいて FAE チームを統括しています。

1992 ~ 1998 年には、エレクトロニクスを専門とする技術者として、ある機械メーカーの部門長を務めていました。ゲッティンゲン応用科学大学で電気工学について学んだ後、マックス・プランク研究所のハードウェア設計技術者としてソーラー・システムの研究に従事しました。2004~ 2010 年には、流通分野の FAE としてアナログ・デバイセズの製品を扱っていました。