How a Wideband O2 Sensor Works | Boosted Technologies, LLC

(REFERENCE FROM: http://www.megamanual.com/PWC/LSU4.htm)

Before one can understand the PWC hardware circuitry and control software, it helps to understand how the wideband oxygen sensor [WBO2] operates (These sensors are also known as universal exhaust gas oxygen sensors [UEGO]).

The Precision Wideband Controller is designed to use the latest ‘wide band’ oxygen sensors. These sensors, when driven by the Precision Wideband Controller’s electronics, can measure the air/fuel ratio directly. Instead of switching back and forth from rich to lean, like conventional “narrow band” exhaust gas oxygen sensor designs, the wide-band sensor produces a signal that is directly proportional to the air/fuel ratio produced by the fuel injection controller. The wide band oxygen sensor responds to changes in the air/fuel mixture in less than 100 milliseconds.

The Precision Wideband Controller circuit is intended to be used to directly control the fuel mixture, so it needs to be accurate and repeatable. When tuning an engine on the road or on a dynamometer, it is desirable to have a means of monitoring engine air-fuel ratio (AFR), which can also be expressed in terms of lambda (λ). During these tuning sessions, engine/vehicle/environmental parameters are kept constant with the exception of the variable being tuned. Wideband meters use a user-interface to obtain the current AFR/lambda so that the engine tuner can adjust and optimize fuel delivery.

The Precision Wideband Controller is a mixture feedback device. A mixture feedback device is used to determine the instantaneous mixture of a running engine, where these parameters are introduced back into the fueling equation in the ECU for real time injector pulse width correction. The main demand of the mixture feedback device is that it needs to be repeatable over absolutely all environmental conditions the same readings for extreme hot or freezing cold conditions. This response is introduced back into the fueling equation in the ECU for real time injector pulse width correction. The main demand of the mixture feedback device is that it needs to be repeatable over absolutely all environmental conditions – the same readings for extreme hot or freezing cold conditions.

In addition, the response function of the wideband UEGO sensors is dependent on parameters like hydrocarbon type, operating temperature, exhaust temperature, exhaust back pressure, etc. If any of these parameters change, then the controller needs to know this and be able to correct/compensate.

Bruce and Al purchased a 5-gas Horiba meter directly from Horiba, so this along with the use of primary gas standards for test gases, lets them know exactly what the sensor sees.

There really is a difference between a wide band EGO meter and a wide band device which directly controls fuel mixture – the mixture device needs to be accurate at all times, or at least be able to notify the mixture control that the WB signal is not within tolerance. Heater control is very import. Steady state running is easy to monitor.

The problems come from events such as recovery after acceleration, where the temperature of the sensor will vary due to changes in exhaust flow. If the sensor temperature changes then the required pump current to maintain equilibrium changes as well (everything else remaining the same) – you either have to keep the sensor temperature regulated or have correction factors – or both (see section 5.1 of the LSU data sheet for a temperature graph with different engine operating conditions and the effect in exhaust temperature).

Throw in transient response for the pump loop, accuracy of the pump measurement circuitry itself, etc. and things can go wrong – and at the wrong time. Getting a handle on all of these effects (and their magnitude) is important for anything that is maintaining a AFR mixture. And the only way to get an handle is to compare against a known calibrated system and a lot of testing.

The wideband air/fuel ratio sensor combines an oxygen-sensing “Nernst” cell from the narrow band sensor with an “oxygen pump” to create a device that gives a wide range response to various air/fuel ratios. The Nernst cell senses exhaust gas oxygen in the same as a conventional narrow band O₂ sensor. If there is a difference in oxygen levels across the ZrO₂ sensor element, current flows from one side to the other and produces a voltage.

The wideband exhaust gas oxygen sensor comes in many constructional forms, but are basically similar in nature. They consist of two parts: a Nernst reference cell and an oxygen pump cell, co-existing in a package that contains a reference chamber and heater element (used to regulate the temperature of the Nernst/pump).

The wide band sensor operates only in combination with specialized wide band control circuits that adjust both the pump cell current and the heater. The Precision Wideband Controller has the required control unit built in to its electronics for a Wide Band Oxygen sensor.

Before delving deeply in the operation of the Nernst and pump cells, it is important to understand what the sensor is actually trying to measure. To start, lets understand the chemical reactions due to combustion.

First, realize that for combustion to occur, there needs to be fuel (such as hydrocarbon) and a source of oxygenates (i.e. oxygen and/or molecules or partial molecules which contain oxygen). In addition, there are diluents which are present in the mixture but do not contribute to the actual combustion (for example, nitrogen [N₂]). This holds true for any combustion event, whether inside of an internal combustion engine or a small campfire.

Second, every atom is conserved in the combustion process, so it is possible to use exhaust gas constituents to reconstruct the amount of fuel and oxygenates before combustion. If this was not the case, then wideband oxygen sensors would not be capable of determining pre-combustion air/fuel ratio.

It is possible to express the combustion event as a balance of input reactants: fuel, oxygenates, and diluents (for example gasoline mixed with air) to the resultant combustion products (i.e. the composition of exhaust gas). Note that this is a chemical balance, meaning that every element needs to be accounted for in its molecular balance, before and after the combustion event. In other words, if we know the proportions of fuel, oxygenates, and diluents entering the engine, one can determine the species composition in the exhaust gas. And we can work backwards. If we know the species in the exhaust we can determine the ratios of air and fuel (both in molar quantity and molecular mass).

Let us represent the chemical composition of the intake fuel as carbon, hydrogen, oxygen, and nitrogen, in proportion of:

^Cα^Hβ^Oγ^Nδ,with α, β, γ, and δ representing the amount of each of the elements present (i.e. moles of each element).

For example, octane has a molecular composition of C₈ H₁₈, so there are 8 atoms of carbon and 18 atoms of hydrogen, so we have α=8, β=18, γ=0, and δ=0.

Other fuel molecules have other compositions, obviously.

Normally, chemists work with a quantity called a “mole”, which is a specific very large number of atoms or molecules of any given species [type]. Combining one mole of atom A, with two moles of atom B is the same as combining one atom of A with two atoms of B, many, many times over.

We can combine the fuel with air and write down a simple balance equation for combustion and balance for the molar quantities before and after combustion:

The items on the left side of the arrow represent the fuel/oxygenates/diluents entering the engine and the items on the right are the molar quantities after the combustion event. We want to solve for the unknown ε, which is the molar fuel-air ratio (equivalency ratio), and the coefficients ν₁, ν₂, and ν₃ that describe the product composition. The variable x_o represents the molar fractional percentage of oxygen in the intake air (0.21 is a commonly used value) and x_n represents the molar fractional percentage of nitrogen (0.79 is often used).

Note that we have more unknowns than equations, so we will have to use some known constraints to help us solve for the unknowns. For one, atoms are conserved (i.e. what goes in must come out), so we can immediately write the following relations (known as the element balance equations):

The solution for the balance equations (listed above) are the following:

And from this one can write the stoichiometric fuel-air mass ratio as:

Note that the stoichiometric mass air-fuel ratio is simply the reciprocal of the above equation. Also, the fuel-air equivalence ratio is defined as the actual fuel-air ratio divided by the stoichiometric fuel-air ratio (note that the reciprocal of this is defined as lambda):

Now, since we are dealing with exhaust gas (i.e. low temperature compared to the actual combustion event) and carbon-to-oxygen ratios less than unity, one can introduce CO and H2 into the balance:

It is somewhat difficult to solve this, but we know a few things can make our life easier. First, if the mixture is lean (i.e. φ < 1) then ν₅ and ν₆ are zero. For rich mixtures, ν₄ = 0. And, for the rich case, we can introduce the watergas equilibrium constant for the reaction:

which yields the constant K_p:

where t is the temperature in Kelvins.

With this, ν₅ can be evaluated as a solution to a quadratic:

where:

Using this result, a chart outlining the solution for each gas species can be tabulated for either lean or rich situations:

There are a few things to note in all of this. First, the hydrocarbon/fuel specified as:

^Cα^Hβ^Oγ^Nδcan be the combination of two or more hydrocarbons. For instance, when fuels are mixed with alcohol, the resulting mixture can be expressed as a single hydrocarbon with balanced subscripts. The same is true for water injection or nitrous oxide injection. This is a very important advantage in using a mathematical approach to determining lambda – if the fuel component changes it is possible to adapt the response of the wideband appropriately without any recalibration. This is not the case with systems that rely on a fixed wideband sensor response “curve”. And, if the wideband controller is connected to a ECU (via CAN bus) and the ECU is controlling the introduction of water or nitrous, it is possible to instantaneously adjust the lambda response curve for any ratiometric combinations of hydrocarbons. This is an important requirement for a mixture controller.

Next, one can divide the hydrocarbon/fuel expression by a constant, which will make the carbon subscript equal to one. This creates a H/C ratio, a O/C ratio, and a N/C ratio – these are often seen in the literature. For example, the fuel C₈H₁₈ (octane) can be normalized to become C₁H_2.25 = CH_2.25, where the H/C ratio is 2.25, the O/C ratio is 0 (because there is no oxygen component) and N/C of 0 (no component), and, of course, the C subscript is 1. Another example is the fuel CH₃NO₂, which already has a C subscript of 1, so the H/C ratio is 3, the N/C ratio is 1 and the O/C ratio is 2. Just note that either form of expressing the fuel is identical.

Note: For those who are interested in experimenting with the above equations, we have developed the program COMBAL, a PC application running under Windows. One basically enters the H/C and O/C ratios, exhaust gas equilibrium, and the target lambda, and it generates the percent moles of each of the gas species. A comparison check using the Brettschneider equation is also performed. The application can be downloaded from:

www.bgsoflex.com/pwb/combal.zipFinally, there are two other gas constituents, CO and H₂, which also exist in the exhaust gas. These are from a balance known as the water-gas equilibrium – more on this later in this document, but suffice to say that it is indeed important in wideband sensor operation.

Are you confused yet? If you are, do not be concerned. All we are outlining here is that with known input fuel, diluents, and oxygenates, one can predict the gas concentrations in the exhaust. And we can go backwards – with measured gas constituents it is possible to determine the input mixture in terms of either lambda or air/fuel ratio. Go back and re-read the section a few times, it is important to understand this aspect.

There is much more to the analysis not shown here – see the Bowling & Grippo paper on the entire analytical method for the Precision Wideband Controller for more info.

The Nernst cell and oxygen pump cell are wired together in such a way that it takes a certain amount of current to maintain a balanced oxygen level in the diffusion gap. Measuring this current flow allows the Precision Wideband Controller to determine the exact air/fuel ratio the engine is operating at.

The pump cell can either consume oxygen or consume hydrocarbon fuel in the pump cell cavity, depending on the direction of the pump cell current flow (I_pump).

In normal sensor operation, exhaust gas passes through the diffusion gap into the pump cell. That exhaust gas is often either rich or lean of stoichiometric. Either condition is sensed by the reference cell which produces a voltage (Vs) above or below the Vref signal, just like a narrow band sensor).

Combustion is rarely perfect though. Even with the correct air/fuel ratio (AFR), combustion can still be incomplete, and CO, H₂, NO_x, and hydrocarbons (HC) can form. This can be caused by quenching (of the flame front against the “cold” surfaces of the combustion chamber), crevice volumes (above the rings between the piston and cylinder), and many other factors.

The relative amounts of these “by-products” change with different air/fuel ratios however.

When the air/fuel mixture is rich, the reference cell produces a high V_s voltage (above 0.450 volts). The Precision Wideband Controller reacts to produce a pump current (I_pump) in one direction to consume the free fuel. The pump cell requires a “negative” current that goes from zero to about 2.0 milliamps when the air/fuel ratio is near 11:1.

When the air/fuel mixture is lean, the reference cell produces a low V_s (lower than 0.450 volts). The Precision Wideband Controller sends the pump current in the opposite direction to consume free oxygen. The pump cell requires a “positive” current that goes from zero up to 1.5 milliamps as the mixture becomes “free air”.

When the air/fuel mixture is 14.7:1 (the stoichiometric ratio for gasoline), the pump cell requires no output current. Since the free oxygen or free fuel has been neutralized by the pump current, the V_s feedback signal goes to about 0.450 volts (the same as the Vref value).

To sense a wide range of air/fuel ratios, the oxygen pump uses a heated cathode and anode to pull some oxygen from the exhaust into a “diffusion” gap between the two components. The pump is driven by two PWM or processor ports in opposite polarity (using either a H-bridge setup or direct processor port drive), and the Precision Wideband Controller measures the time when the reference cell passes through 0.45 volts. It can then adjust the PWM timing to bracket this 0.45 volt stoichiometric flipping point.

Like a conventional narrow band sensor, the Precision Wideband Controller circuit produces a low-voltage signal when the air/fuel ratio goes lean, and a high-voltage signal when the mixture is rich. But instead of switching abruptly at stoichiometric, it produces a proportional change in the voltage. It increases or decreases in proportion to the relative richness or leanness of the air/fuel ratio. With a stoichiometric air/fuel ratio of 14.7:1, the wide-band O2 sensor will produce a steady 0.450 volts. If the mixture goes a little richer or a little leaner, the sensor’s output voltage will only change a small amount instead of rising or dropping dramatically.

The result is a sensor element that can precisely measure air/fuel ratios (AFR) from very rich (10:1) to extremely lean (free air). This allows the Precision Wideband Controller to control the air/fuel ratio directly. Instead of switching the air/fuel ratio back and forth from rich to lean to create an average balanced mixture, the PWC can simply add or subtract fuel as needed to maintain a stoichiometric ratio of 14.7:1 or any other ratio.

Another difference between the narrow band sensor found in most automobiles and the wide band oxygen sensor is in the heater circuit. The heater power is closed loop controlled while the measurement is done, so that a nominal sensor internal resistance of R_i=80 Ohms (measured with 1 to 4 kHz) is reached, this corresponds to a sensor ceramic temperature of approx. 750°C when the sensor is new. The Precision Wideband Controller (PWC) heater circuit is modulated to maintain a consistent operating temperature of 1300°F to 1500°F (700°C to 800°C). The sensor takes about 20 seconds to reach operating temperature from a cold start.

The sensor incorporates a 10 Watt (3.2 ohms at 20°C, 2.1 ohms at -40°C) heater that ensures the sensors is kept at the nominal operating temperature of 750°C (~1400°F). The current to the heater is limited by the Precision Wideband Controller circuitry to prevent excessive heating during warm-up. The sensor heater must never be connected directly to battery voltage, it must always be controlled by the Precision Wideband Controller. Starting the sensor heating before engine start is not advisable, it will harm the sensor.

The maximum operating exhaust gas temperature for the sensor is up to 850°C (1560°F). If the maximum exhaust gas temperature is exceeded, the heater power must be switched off, and the accuracy of the sensor signal is reduced. Hot exhaust gas with a temperature above the operating temperature of the ceramic gives also a deviation of the ceramic temperature and the sensor output signal. Cold exhaust gas, in addition with high gas velocity, can lead to a reduced sensor ceramic temperature, if the heater control is not able to keep the constant ceramic temperature. This leads to a deviation of the sensor output signal. As a general rule, a temperature change of the sensor ceramic gives a deviation of the sensor output signal of:

(ΔI_pump)/I_pump of approx. 6%..7% / 100K.Lets move on. Now lets attempt to understand the operation of the Nernst cell section of the UEGO. The Nernst cell is an electrochemical cell consisting of a solid electrolyte conductive only to oxygen ions. Attached to this electrolyte are two platinum electrodes. One electrode is exposed to atmosphere and the other is exposed to a reference chamber (more on this later).

At the electrodes, the following reactions occurs:

With this reaction occurring, a current can be generated. Using the Nernst equation, one can calculate the EMF produced under a no-load situation:

Where E is the Nerstian EMF generated,
R is the Universal Gas Constant = 8.31 J*K^-1*mol^-1,
T is the temperature of the cell in Kelvin,
F is the Faraday Constant = 96500 Cmol^-1,
Z is the electrons transported per O₂ = 4.

Because there is a heater maintaining the Nernst cell at an elevated temperature, a temperature gradient exists which generates an offset voltage. We can add this term to the above term, and in the process we can also simplify the calculation by converting from base e to base 10 logarithms:

Now that we know the operation of the Nernst cell, a little on the physical construction is in order. The UEGO sensor is of a “planar structure” – this means that it is in a rectangular form as opposed to a thimble or other symmetrical shape – think of a flat sandwich of components. In the sandwich, there is the Nernst electrolyte which is generally constructed from Yttria Stabalized Zirconia (YSZ), although other forms do exist. What is Yttria Stabilized Zirconia? It is Zirconia (ZrO₂) with roughly three percent of moles substituted with Yttria (Y₂O₃). Because every two zirconium ions are replaced with yttrium, an oxygen vacancy exists – this allows adjacent oxygen ions to “jump” to these sites and at elevated temperatures this activity is the basis for EMF production.

Continuing the discussion of the planar structure, there exists an internal “diffusion cavity” – this cavity is where the sample of exhaust gas is “trapped”, as well as where the Nernst and pump sections face. How does the gas get there? By a diffusion process, the exhaust gas to be sampled enters the cavity. Not to get too “geeky” about the diffusion process, but suffice to say that there are two diffusion mechanisms:

one is known as molecular diffusion, and
the second is known as Knudsen diffusion, or “fine-pore” diffusion.

It is very important to note: Knudsen diffusion is temperature dependent – this means that the porosity of the test chamber (i.e. how much gas can enter/exit) depends on the sensor head temperature – this is why pumping current (described next) is different for different temperatures, as well as exhaust back pressure dependence.

The aforementioned oxygen pump – this is what makes a run-of-the-mill oxygen sensor a true wideband unit – is really just another Nernst-type cell with an external current applied to it.

We talked about the “cavity” above where sample exhaust gas exists and on one side is the Nernst measurement cell. On the other side is the pump cell – this cell is used to transport oxygen into and out of the measurement cavity. In very simplistic terms, if the exhaust gas in the measurement cell is lean, then there is excess oxygen (lean mixtures mean excess oxygen). We can “turn on the pump” to remove oxygen from the reference cavity – and with the proper feedback monitoring of the Nernst measurement cell we can pump out just enough oxygen to achieve a stoichiometric balance (roughly when the Nernst measurement cell reads 0.45 volts or thereabouts).

The best part of all: if we monitor the pump current, we can use this to determine lambda (λ) and AFR Pump current is related to the amount of oxygen pumped out as a function of time as:

with n being the moles of O₂ gas pumped, t for time and current i. To make this equation useful it should be converted to partial pressure change within the reference cavity. Also note that the diffusion (explained above) will bring in more exhaust gas over time – so what we are doing is making an equilibrium with feedback from the Nernst measurement cell dictating how much oxygen to pump away, all the while more exhaust gas is diffusing in. Note that the pressure of the exhaust gas under measurement also affects the amount of diffusion into and out of the measurement cavity – this is the famous back pressure effect.

We have explained the excess-oxygen case where the air-fuel mixture is lean. How does it operate on the oxygen-depleted side, or rich air/fuel ratio side? For this case, oxygen is ‘pumped’ into the measurement cavity simply by reverse application of current on the pump element. Feedback on the Nernst measurement cell indicates when stoichiometric equilibrium has been achieved.

Now, something should be bothering your gut right about now…

The pump cell operates on oxygen ion transport, but we are in a situation where there is no oxygen in the air-fuel mixture (i.e. we are rich). If we become much more rich, we still do not have oxygen. Super rich, and still no oxygen. How can there be a feedback situation in this case?

It turns out that within the diffusion measurement cavity, the following chemical reactions are occurring:

So, the oxygen pumping portion acts to introduce the oxygen into the diffusion chamber by the electrolysis decomposition of the carbon dioxide (CO₂) and water (H₂O) in the measuring gas. Think of it this way: we have exhaust gas trapped in the diffusion cavity which contains H₂ and CO, and the oxygen pump is generating O₂ – these combine to produce CO₂ and water. If we have more H₂ and CO in the exhaust gas, then more O2 from the pump gets converted – and, in order to increase O₂ production we increase the pump current.

And it turns out that H₂ and CO are present in significant amounts for a rich AFR, and can be related to lambda by the elemental balance equation for the fuel/oxygenates/diluents we derived above.

This is not exactly right, in that we are dealing with a gas balance and the pump is really an electrochemical cell (click on the links for background information on Le Châtelier’s Principle for equilibrium balance rules, as well as the Ideal Gas Law), so we need the oxygen in the H₂O and CO₂ as donors for the reaction – this where the pump gets its oxygen. It is a balance, and by changing the amount of current pumped into the pump we can change the balance. The balance is also driven by the water-gas reaction, discussed later on.

Finally, lambda (λ), what we all want to know, is related to all of the exhaust gas components in simplistic relation known as the Brettschneider equation:

All this says is that there are known combinations of exhaust gas quantities (either in terms of moles or in partial pressure) that directly relate to lambda. These include H₂ and CO.

So, armed with all of this knowledge, we can write an equation relating pump current compared to exhaust gas component, then stick this into the Brettschneider equation (or a more advanced form – see the Bowling & Grippo paper). For the lean mixture side where there is excess oxygen, the pump current equation is:

So, the required pump current I_p is simply the partial pressure of O₂ in the diffusion chamber multiplied by a calibration coefficient K_o2. Remember, this is the partial pressure of oxygen, not the molar quantity, so the elemental mass needs to be involved.

For the rich mixture side, where there is no oxygen, the sensor measures the amount of CO and H₂ in the exhaust gas (partial pressure):

Note the minus signs. The applied pump current is reverse polarity such to make the oxygen pump an oxygen generator, not an oxygen “sucker”.

Also note that on the rich side, the UEGO sensor reacts to unburned hydrocarbons as well. However, in normal combustion, the amount of unburned hydrocarbons are in the parts per million region, whereas the moles of CO and H₂ are substantially higher (like in the 10 – 20% range).

Measuring the Nernst Cell Resistance

Accurate temperature control of the wideband UEGO probe is an absolute requirement during operation. Changes in UEGO probe temperature will result in a change in required pump current (from the difference in diffusion in and out of the measurement cavity), so monitoring the temperature allow for corrections to be applied to the measurements. The wide band sesnor does not have any form of direct temperature measurement (i.e. thermistor,thermocouple, etc.).

However, monitoring the resistance of the reference cell yields a close representation of the probe temperature – the resistance of the reference cell varies with temperature. The Nernst reference cell has a high resistance at low temperatures (i.e. ambient temperatures) and a resistance of approximately 80-100 ohms at normal operating temperature. So, by monitoring the internal resistance of the reference cell it is possible to determine an accurate UEGO probe temperature, without the need of an external temperature sensor element.

There are several methods available to measure the resistance of the reference cell, including disabling the pump circuit and applying a known constant current across the reference cell and measuring the resultant voltage, finally re-enabling the pump circuit. This method requires several analog switches to apply the current and re-establish the pump servo circuit when done. Also, if a bias is applied to the Nernst cell, then an opposite polarity current with the same duration needs to be applied in order to “reset” the polarization on the cell. The one problem with this method is that it is “intrusive” to the feedback loop of the Nernst/pump.

Another method is to apply a high-frequency waveform to the pump circuit and measure the resultant deviation in EMF. The reference cell’s resistance is determined by AC-coupling a square wave of known amplitude and frequency via a series resistance, and measuring the resultant AC waveform’s amplitude. This waveform is always present, and since it is at a high frequency with respect to the response of the Nernst/pump feedback loop, it essentially averages out. This is the method employed in the PWB.

Circuit operation is very simple. A known square-wave source of 5 volts peak-to-peak and at a frequency of 1 to 3 KHz (generated by the DSP) is capacitively coupled to the reference cell positive terminal. Overall current is limited by a series resistance (plus R_i internal resistance) to 500 microamps peak to peak, or ±250 microamps around the V_bias point (V_bias is set to 2.5 volts to allow for bi-polar pump operation) – this value meets the specification outlined in the Bosch LSU 4.2 data sheet. The alternating current signal generates a corresponding alternating voltage with value based on the internal resistance R_i. For example, if R_i = 100 ohms, then 500 microamps (P-P) multiplied by 100 ohms yields 50 millivolts p-p, or ±25 mv around the V_bias point. Actually, the series current limit resistance and R_i form a resistor divider circuit driven by a voltage potential.

To measure the voltage, a capacitor is used to block the DC offset (i.e. reference cell voltage) and pass the alternating signal. A gain stage is introduced and the voltage is fed into a A/D port on a processor. Note that this signal is an AC signal, so ADC sampling needs to correlate with the polarity of applied square wave signal – this is known as synchronous rectification. An alternative method would be to use a bridge rectifier circuit to recover the positive/negative swings and then filter before application to the ADC channel.

Leaded Fuel

Wideband oxygen sensors are designed for an operational life of 100,000 miles (160,000 kms) under normal operating conditions. Replacement is required only if the sensor has failed due to unusual operating conditions, physical damage, or contamination. For example, a blown head gasket might allow silicon to enter the exhaust and contaminate the sensor. Oil burned in the combustion chamber due to leaking valve guides or rings can allow phosphorus to enter the exhaust and contaminate the sensor.

Depending on the lead contents of the used fuel, the expected service life time is:

for 0.6 g Pb/l: 20,000 km (12,000 miles)
for 0.4 g Pb/l: 30,000 km (18,000 miles)
for 0.15 g Pb/l: 60,000 km (36,000 miles)

In general, when using leaded fuel, the sensor will need to be replaced when functional problems occur, e.g. instable idle speed, driveability problems. The following tests can be done for a rough check of the sensor function:

Reasonableness of the signal check in rich exhaust gas: sensor signal should indicate rich
Reasonableness of the signal check in “free-air”: sensor signal should indicate very air lean
Heater cold resistance at room temperature, with a multimeter between grey and white cable (H+, H-), and the sensor not connected to the Precision Wideband Controller, should be 2.5 to less than 10 ohms

* We dedicate the Precision Wideband Controller to the memory of Garfield Willis. Garfield was instrumental in early research and development of the EGOR wideband controller.

Last Updated: 05/04/2020 09:45:16

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