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CHAPTER 16. FOUNDATION FIELDBUS INSTRUMENTATION

16.6H1 FF segment troubleshooting

Feedback obtained from industrial users of FF reveal a common pattern: Fieldbus is a powerful and reliable technology, but only if it is properly installed. Poor installations, usually driven by a desire to minimize capital expenses, will cause numerous problems during commissioning and operation.

One relatively easy way to avoid problems caused by short-circuits in FF wiring is to use coupling devices with built-in short-circuit protection. This feature does not add significant cost to the coupling device, and it will prevent the entire segment from failing due to a short-circuit on a single spur cable or within a device. Use coupling devices with indicator LEDs as well, since these give easy visual verification of network power which may greatly accelerate FF segment troubleshooting when the need arises.

16.6.1Cable resistance

A simple check of an H1 segment’s cabling consists of a series of resistance measurements performed with the segment unpowered (as is standard with any electrical resistance check), with all FF devices disconnected, and with the cable entirely disconnected (all three conductors) at the host end. The following table shows guidelines published by the Fieldbus Foundation for H1 segment cable resistance measurements:

Measurement points

Expected resistance

Between (+) and (−) conductors

> 50 kΩ, increasing over time

Between (+) conductor and shield (ground)

> 20 MΩ

Between (−) conductor and shield (ground)

> 20 MΩ

Between shield conductor and earth ground

> 20 MΩ

The last resistance check shown in the table checks for the presence of ground connections in the shield conductor other than the one ground connection at the host end (which has been disconnected for the purposes of the test). Since the shield should only be grounded at one point26 (to avoid ground loops), and this one point has been disconnected, the shield conductor should register no continuity with earth ground during the test.

The necessity of disconnecting all FF devices and host system interfaces is essential so that the resistance measurements reflect the health of the cable and nothing else. The presence of any FF devices on the segment would substantially a ect the resistance measurements, particularly resistance between the signal (+ and −) conductors.

26An alternative method of shield grounding is to directly connect it to earth ground at one end, and then capacitively couple it to ground at other points along the segment length. The capacitor(s) provide an AC path to ground for “bleeding o ” any induced AC noise without providing a DC path which would cause a ground loop.

16.6. H1 FF SEGMENT TROUBLESHOOTING

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16.6.2Signal strength

The Fieldbus Foundation specifies a signal voltage (peak-to-peak) range of 350 mV to 700 mV for a healthy FF segment. Excessive signal voltage levels point to a lack of terminator resistor(s), while insu cient voltage levels point to an over-abundance of terminators (or perhaps even a device short):

Signal voltage (pk-pk)

Interpretation

 

 

800 mV or more

Possibly missing terminator resistor

350 mV to 700 mV

Good signal strength

 

 

150 mV to 350 mV

Marginally low signal – possible extra terminator resistor(s)

150 mV or less

Too little signal to function

 

 

16.6.3Electrical noise

FF, like all digital networks, are una ected by noise voltage below a certain threshold. If noise voltage is present in excessive quantity, though, it may cause bits to be misinterpreted, causing data errors. The Fieldbus Foundation gives the following recommendations27 for noise voltage levels on a FF segment:

Noise voltage (pk-pk)

Interpretation

 

 

25 mV or less

Excellent

25 mV to 50 mV

Okay

 

 

50 mV to 100 mV

Marginal

100 mV or more

Poor

 

 

Fieldbus diagnostic tools measure noise on the network segment during times between message frames, when there should be purely DC voltage between the two conductors.

27Bear in mind the tolerable level for noise will vary with signal voltage level as well. All other factors being equal, a strong signal is less a ected by the presence of noise than a weak signal (i.e. the signal-to-noise ratio, or SNR, is crucial).

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CHAPTER 16. FOUNDATION FIELDBUS INSTRUMENTATION

16.6.4Using an oscilloscope on H1 segments

A tool available in most instrument shops is a digital-storage oscilloscope, which may be used to measure and display FF H1 signal waveforms for analysis of problems. Analog oscilloscopes are also useful for network troubleshooting, but to a lesser degree28.

When using an oscilloscope to measure FF H1 signals, it is very important not to connect either of the FF segment conductors to earth ground through the oscilloscope. Introducing such a “ground fault” to the network segment will almost certainly cause communication problems, in addition to whatever problems already exist that compel you to diagnose with an oscilloscope. If a single channel of the oscilloscope is connected across the segment wires, the “ground” clip of the probe will force one of those conductors to earth ground potential via the metal chassis of the oscilloscope which is grounded through the third prong of the power plug for safety. An exception to this rule is if the oscilloscope itself is battery-powered and has an insulated case where no ground connection is made through the surface it sits on or the human hand that holds it. Otherwise, using a single channel on a line-powered oscilloscope to measure network signals is inviting trouble.

28It is impossible to “lock in” (trigger) non-periodic waveforms on an analog oscilloscope, and so most network communications will appear as an incomprehensible blur when viewed on this kind of test instrument. Digital oscilloscopes have the ability to “capture” and display momentary pulse streams, making it possible to “freeze” any portion of a network signal for visual analysis.

16.6. H1 FF SEGMENT TROUBLESHOOTING

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If a line-powered oscilloscope must be used, the proper way to configure it is for di erential channel measurement. In this mode, the oscilloscope will register the voltage between two probe tips, rather than register the voltage between a single probe tip and earth ground.

Power conditioner

100 Ω 10 mH

Fieldbus junction box

Fieldbus junction box

 

 

100 Ω

Trunk cable

Trunk cable

100

Ω

 

 

 

 

24 VDC

1

μF

 

 

 

 

 

 

 

 

 

 

Terminator

 

 

 

1 μF

 

 

 

 

 

Terminator

 

 

 

 

Spur cable

 

 

 

 

 

 

 

Spur cable

 

H L

FF transmitter

 

 

 

 

 

 

 

 

Sec/Div

FF valve

Volts/Div A

 

 

 

 

 

positioner

0.5

0.2

0.1

 

 

 

 

 

1 m

250 μ 50 μ

1

 

50 m

Position

 

 

 

 

5 m

 

10 μ

2

 

20 m

 

 

 

 

25 m

 

2.5 μ

 

5

 

10 m

 

 

 

 

 

100 m

 

0.5 μ

 

10

 

5 m

 

 

 

 

 

500 m

 

0.1 μ

 

20

 

2 m

 

 

 

 

 

1 2.5

 

off 0.025 μ

 

 

 

DC Gnd AC

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

X-Y

 

 

 

A

B

Alt Chop Add

 

 

 

 

 

 

Position

 

 

 

 

 

Triggering

 

 

 

 

 

 

 

 

 

 

Level

 

 

 

 

 

 

 

 

 

A

 

 

 

Volts/Div B

 

 

 

 

 

B

 

Holdoff

 

 

 

 

 

 

Alt

 

 

0.5

0.2

0.1

 

 

 

 

 

Line

 

 

 

1

 

50 m

Position

 

 

 

 

 

 

 

2

 

20 m

 

 

 

 

 

Ext.

 

Ext. input

 

5

 

10 m

Invert

Intensity

Focus

 

Norm

AC

 

 

10

 

5 m

Beam find

 

 

 

 

 

DC

 

 

 

20

 

2 m

 

 

 

 

Auto

 

 

 

 

 

DC Gnd AC

Off

 

 

Single

Slope

 

LF Rej

 

 

 

 

 

Cal 1 V Gnd

Trace rot.

Reset

 

HF Rej

 

 

 

 

 

 

 

 

 

 

 

 

Oscilloscope

 

 

 

 

Configuring a dual-trace oscilloscope for di erential mode is quite simple. On the front panel of the oscilloscope, you must set the multi-trace controls to the Add mode, where one trace on the screen represents the instantaneous sum of the two inputs (channels “A” and “B”). The volts per division “sensitivity” of both channels should be set to exactly the same value. Also, the Invert control must be engaged for the second input channel, forcing that channel’s signal to be inverted (register upside-down on the screen). The summation of channel “A” and an inverted channel “B” is equivalent to the mathematical di erence (subtraction) between “A” and “B,” which means the single trace on the screen now represents the di erence of potential between the two probe tips. The oscilloscope now behaves as an ungrounded voltmeter, where neither of the test leads is referenced to earth ground.