Background Image
Table of Contents Table of Contents
Previous Page  36 / 40 Next Page
Information
Show Menu
Previous Page 36 / 40 Next Page
Page Background

Chemical Technology • July 2015

34

CONTROL & INSTRUMENTATION

with high water content in the past. In the

case of these measuring devices, the high

CO

2

content typically present in biogas

flows had a negative effect on the measur-

ing stability since the molecular structure

of the carbon dioxide can significantly

decrease the dispersion of the ultrasonic

signals. In addition, the cost to purchase

these devices is still comparatively high,

which often made the use of ultrasonic

flowmeters unattractive in the past.

Nevertheless, based on their design,

ultrasonic flowmeters have always been

particularly well suited to biogas appli-

cations as they guarantee a full transit

without loss of pressure or any negative effect on the flow

and they can cover a wide measuring range.

Innovative ultrasonic flow measuring

technology for biogas

Much has been learned in measuring technology from the

experience with biogas applications. This is especially true

in the area of ultrasonic flowmeasuring technology. Through

investment, research and development, leading measuring

technology manufacturers have managed to produce a

new generation of ultrasonic flowmeters that specifically

targets the high requirements of biogas applications. The

fact that ultrasonic technology has helped make measuring

the flow of biogas manageable while remaining affordable

is illustrated, for example, by Krohne’s new OPTISONIC

7300. The device offers a series of new functions for biogas

measurement while remaining completely competitive as

regards procurement cost.

The measuring instrument, which functions according

to the time transit differential method, guarantees flow

measurement with a high degree of long term stability

regardless of the gas composition. The solution is mainte-

nance-free and immune to deposits. Thanks to its special

signal converter design, the OPTISONIC 7300 also features

considerably higher signal strength. The NACE approved

Grade 29 Titanium transducers provide excellent corro-

sion resistance against H2S. An enhanced digital signal

processor (DSP) also allows for better detection of small

acoustic signals strongly dampened by high CO

2

content.

In addition, its transducer and transducer pocket design

make it insensitive to liquid water. In this way old sources

of error are eliminated from the start.

The OPTISONIC 7300 does not have limitations such as

regular recalibrations, pressure loss or limited flow range. In

addition, to make various measurements comparable, the

standard volume can be measured following the input of

temperature and pressure using the OPTISONIC converter.

The measuring device also features an integrated calcula-

tion of the methane content (see box above).

Practical experience with the OPTISONIC has shown

after a short period of time how stable and accurately

biogas measurements can now be performed. Exactly how

operators of biogas plants can use this to their advantage

is clearly illustrated by the application example of the Ara-

bern wastewater treatment plant shown in the box above.

z

Calculation of the methane content at the wastewater treatment plant in the Ara Region Bern,

Switzerland

The molar mass (M) of a gas can be determined according to the fol-

lowing formula which is implemented in the OPTISONIC 7300.

γ = Adiabatic index, pre-set value into the flowme-

ter electronics; an average value of 1,31 is entered

for the CO

2

/CH4 mixture.

R = Molar gas constant, approx 8,3145 J mol–1

K–1.

T actual = Gas temperature in Kelvin, can be

measured via a 4–20 mA input on the converter

VoS = Sound velocity of the gas

The methane content can be

calculated from the molar mass,

considering the following: The

molar weight of CO

2

(44)

Themolarweight ofmethane (16)

The molar weight of water (18)

The amount of water in the gas

depends on the temperature.

For a water saturated gas the

amount of water is known.

M= y RT actual

VoS

2

Figure 1: Velocity of sound/methane

content at 30°C

The methane content is measured with an accuracy of 2 % (including

uncertainty of the temperature measurement of 1 %).

Figure 3: Amount of water

in a gas depending on the

temperature

Figure 2: Composition of biogas depends on the molar weight