Calculation will run with almost 2-fold (Dual Core) or 4-fold (Quad-Core) the speed.
Calculation will run up to 16-fold the speed. (Requires multiple networked sufficient PCs; Special Installation knowledge required.)
Dispersion area types I to
V
Area maps for types I to
V
Dispersion area types VI to
IX
Area maps for types VI to
IX
Dispersion area types X to XVIII
Dispersion area types X to XII
Area maps for types X to
XII
Dispersion area types XIII to XV
Area maps for types XIII to
XV
Dispersion area types XVI to XVIII
Area maps for types XVI to
XVIII
Dispersion area types XIX to XXI
Area maps for types XIX to
XXII
Area maps for types XXIII to XXV
Table of input data for
instantaneous release
Table of input data for continuous
release
This type of dispersion area can be used for accidental releases in flat terrain without obstacles. Furthermore, it can replace all the dispersion areas with obstacles which lead to a reduction of the concentration if no special diagrams are available.
This type of dispersion area can be used for accidental releases in which the dispersion is limited by an obstacle to a hemisphere. The obstacle can consist of a row of buildings, a dam, a dock or similar objects near the source. This type of dispersion area may also be used for shorter obstacles or other heights at larger distances, if no other special diagrams are available. If the distance of the obstacle amounts to more than 5 Lei (for instantaneous release) or 30 Lee (for continuous release), the effect of the obstacle on the heavy gas dispersion can be disregarded.
This type of dispersion area can be used for accidental releases for which the dispersion is limited by an uninterrupted canyon of orthogonal walls which is parallel to the wind. This type of dispersion area can also be used for canyons of other geometries if no other special diagrams are available therefore. Deeper canyons lead to similar concentrations. For lower, broader or interrupted canyons, it will yield conservative estimations. For single, interrupted buildings, the (*UZD) lower flammability distances are considerably overestimated if the diagram of dispersion area type III is used.
For this type of dispersion area, a hemispherical, impermeable protective wall is located at such a distance leeward of the source that a distinct protection is obtained for those locations which are situated beyond the wall. On the bases of the results, the potential protection effect of such a measure can be estimated.
In contrast to dispersion area type IV, the protective wall is placed nearer to the source for this type of dispersion area, and the protecting effect decreases.
Flat terrain without obstacles.

Flat terrain. This dispersion is limited to a hemisphere by a wall located near the source and parallel to the wind (Fig. 2). The wall is located at a distance of 1 Lei (for instantaneous release) or 5.6 Lee (for continuous release) from the gas source. The wall is to be regarded as infinitely long and, during the heavy gas spread phase, as infinitely high (1Lei or 5.6 Lee).

Flat terrain. This dispersion takes place in a canyon of orthogonal walls. This canyon has a height of 1 Lei (for instantaneous release) or 7 Lee (for continuous release), and a breadth of 2 Lei or 28 Lee, respectively.

Flat terrain. Semi-circular, massive wall leeward of the source. The height of the wall is 0.4 Lei (for instantaneous release) or 2.24 Lee (for continuous release). The distance between the source and the obstacle amounts to 4 Lei or 22.4 Lee, respectively.

Flat terrain. Semi-circular, massive wall leeward of the source. The height of the wall is 0.4 Lei (for instantaneous release) or 2.24 Lee (for continuous release). The distance between the source and the obstacle amounts to 2.5 Lei or 14 Lee, respectively.

In this dispersion area the wall, already used in dispersion area V, was placed in winward of the source. In contrast with the wall leeward of the source, in the dispersion area V no distinct protection is visible. The concentrations, however, are below those concentrations measured in the area without obstacles. As a reason for this, the shade of the area near the source is to be mentioned. This causes a stronger lateral dispersion of the gas cloud.
The wall used in this dispersion area corresponds to the obstacle used in the dispersion area IV. Just as in the dispersion area VI, the wall was placed here winward of the source. Although the concentrations are lower here than in the dispersion area without obstacles, not a significant protection is obtained by this obstacle.
The obstacle in this dispersion area is in principle a combination of the obstacles used in the dispersion area types V and VI. The circular, impermeable protective wall with the source in the center used here, shows a great distinctive protection for all the locations situated downstream of the source leeward of the protection wall. The position of the protective wall is clearly the cause of the strong concentration gradient. As on the basis of the shade within the protective wall, the gas can spread stronger laterally than in the dispersion area type V, the concentration in the dispersion area VII is generally lower than in the dispersion area type V.
The circular, impermeable protective wall in this dispersion area corresponds to a combination of the obstacles in the dispersion area IV an VII. Also, as in the dispersion area type VIII, a great distinct protection for locations situated downstream of the source leeward of the protection wall is visible.
Flat terrain. Semi-circular, massive wall windward of the source. The height of the wall is 0.4 Lei (for instantaneous release) or 2.24 Lee (for continuous release). The distance between the source and the obstacle amounts to 2.5 Lei or 14 Lcc, respectively.

Flat terrain. Hemispherical, massive wall in luv of the source. The height of the wall is 0.4 Lei (for instantaneous release) or 2.24 Lee (for continuous release). The distance between the obstacle and the source amounts to 4Lei or 22.4 Lcc, respectively.

Flat terrain. Circular, massive wall around the source. The height of the wall is 0.4 Lei (for instantaneous release) or 2.24 Lee (for continuous release). The distance between the source and the obstacle (radius of the obstacle) amounts to 2.5 Lei or 14 Lcc, respectively.

Flat terrain. Circular, massive wall around the source. The height of the wall is 0,4 Lei (for instantaneous release) or 2,24 Lee (for continuous release). The distance between the source and the obstacle (radius of the obstacle) amounts to 4 Lei or 22,4 Lcc, respectively.

The dispersion area types X to XVIII can be used for accidental releases in which the dispersion is limited by an interrupted canyon of orthogonal walls which is parallel to the wind.
In case of an instantaneous release the measured mean UZD are generally
lower in these dispersion areas than the UZD measured in an uninterrupted
canyon (dispersion area type III). In the dispersion area type X (in continuous
release) after 50 Lee distance from the source, lower UZD than in
the dispersion area type III are visible, while the UZD in the dispersion area
types XI and XII are generally lower than the values measured in the dispersion
area type III.
The greater dilution of the heavy gas cloud is traced back to
the greater mixing with ambient air. This is caused by the lateral building
gaps.
As it is evident from the concentration courses, a widening of the canyon and the building gaps leads to a reduction of the UZD values.
Flat terrain. The dispersion takes place within a canyon of orthogonal
walls interrupted by lateral gaps. It is 1.5 Lei (for instantaneous
release) or 11 Lee (for continuous release) high and 2
Lei or 14 Lee wide.
The lateral walls of the canyon
consist of pieces which are 15 Lei or 105 Lee long and
separated from each other by gaps which are 2 Lei or 14
Lee wide.
The source is located in the center of the canyon and
in the center of a building gap.

Flat terrain. The dispersion takes place within a canyon of orthogonal
walls interrupted by lateral gaps. It is 1.5 Lei (for instantaneous
release) or 11 Lee (for continuous release) high and 3
Lei or 21 Lee wide.
The lateral walls of the canyon
consist of pieces which are 15 Lei or 105 Lee long and
separated from each other by gaps which are 3 Lei or 21
Lee wide.
The source is located in the center of the canyon and
in the center of a building gap.

Flat terrain. The dispersion takes place within a canyon of orthogonal
walls interrupted by lateral gaps. It is 1.5 Lei (for instantaneous
release) or 11 Lee (for continuous release) high and 4
Lei or 28 Lee wide.
The lateral walls of the canyon
constist of pieces which are 15 Lei or 105 Lee long and
separated from each other by gaps which are 4 Lei or 28
Lee wide.
The source is located in the center of the canyon and
in the center of a building gap.

This dispersion area types can be used in principle for the same canyons as the dispersion area types X, XI and XXII, though with a source of different location. As well as in the area types X to XII, a widening of the canyon and the building gaps lead to a reduction of the UZD values.
In case of an instantaneous release the mean UZD values of the area types XIII to XV are generally lower than the UZD measured in the dispersion area type III. In the dispersion area types XIII, XIV and XV (in instantaneous release) the mean concentration values after a source distance of a maximum of15 to 20 Lei are already lower than in an area without obstacles.
In case of a continuous release, the measured mean UZD values in the range of 50 to 200 Lee in the area types XIII to XV drop below the values measured in the area type III. However, during the entire heavy gas spread phase, those values are greater than the values measured in the area without obstacles.
Flat terrain. The dispersion takes place in a canyon of orthogonal walls
interrupted by lateral gaps. It is 1.5 Lei (for instantaneous
release) or 11 Lee (for continuous release) high and 2
Lei or 14 Lee wide.
The lateral walls of the canyon
consist of pieces which are 15 Lei or 105 Lee long and
separated from each other by gaps which are 2 Lei or 14
Lee wide.
The source is located in the center of the canyon
between two building gaps.

Flat terrain. The dispersion takes place within a canyon of orthogonal
walls interrupted by lateral gaps. It is 1.5 Lei (for instantaneous
release) or 11 Lee (for continuous release) high and 3
Lei or 21 Lee wide.
The lateral walls of the canyon
consist of pieces which are 15 Lei or 105 Lee long and
separated from each other by gaps which are 3 Lei or 21
Lee wide.
The source is located in the center of the canyon
between two building gaps.

Flat terrain. The dispersion takes place within a canyon of orthogonal
wall interrupted by lateral gaps . It is 1.5 Lei (for instantaneous
release) or 11 Lee (for continuous release) high and 4
Lei or 28 Lee wide.
The lateral walls of the canyon
consist of pieces which are 15 Lei or 105 Lee long and
separated from each other by gaps which are 4 Lei or 28
Lee wide.
The source is located in the center of the canyon
between two building gaps.

These dispersion areas can be used in principle for the same canyons as the dispersion area types X, XI and XII. However, the location of the source is moved upstream to the beginning of the building gap. A widening of the canyon and the building gaps leads to a reduction of the UZD values.
In instantaneous releases as well as in continuous releases, the mean
UZD values measured in these areas are generally lower than the values measured
in the dispersion area type III. In the dispersion area types XVI and XIII in
instantaneous release, the mean UZD values are generally lower when there are
no obstacles. This is also valid in case of continuous release for the
dispersion area type XIII.
The mean UZD values are generally greater in the
dispersion area type XI than in the dispersion area without obstacles. In the
dispersion area type XVII the mean UZD values are at first lower than in the
case without obstacles. Because of the reduced lateral dispersion of the cloud,
the dilution proceeds slower than in the case without obstacles; and so the
mean UZD values in the dispersion area type XVII from about 150 Lee
distance from the source, are greater than the values measured in the area type
I.
Flat terrain. The dispersion takes place within a canyon of orthogonal
walls interrupted by lateral gaps. It is 1.5 Lei (for instantaneous
release) or 11 Lee (for continuous release) high and 2
Lei or 14 Lee wide.
The lateral walls of the canyon
consist of pieces which are 15 Lei or 105 Lee long and
separated from each other by gaps which are 2 Lei or 14
Lee wide.
The source is located in the center of the canyon at
the beginning of a building gap.

Flat terrain. The dispersion takes place within a canyon of orthogonal
walls interrupted by lateral gaps. It is 1.5 Lei (for instantaneous
release) or 11 Lee (for continuous release) high and 3
Lei or 21 Lee wide.
The lateral walls of the canyon
consist of pieces which are 15 Lei or 105 Lee long and
separated from each other by gaps which are 3 Lei or 21
Lee wide.
The source is located in the center of the canyon at
the beginning of a building gap.

Flat terrain. The dispersion takes place within a canyon of orthogonal
walls interrupted by lateral gaps. It is 1,5 Lei (for instantaneous
release) or 11 Lee (for continuous release) high and 4
Lei or 21 Lee wide.
The lateral walls of the canyon
consist of pieces which are 15 Lei or 105 Lee long and
separated from each other by gaps which are 4 Lei or 28
Lee wide.
The source is located in the center of the canyon at
the beginning of a building gap.

The dispersion area types XIX to XXI can be used for accidental releases, in which the dispersion takes place within an area of interrupted uniform buildings.
In instantaneous as well as in continuous release, the mean UZD values
measured in these dispersion area types are lower than the values measured in
the area without obstacles (area type I). The greater dilution is traced back
to the greater mixing with ambient air caused by the buildings.
As it is
evident from the concentration courses, a further interruption of the buildings
leads to rising UZD values until finally the UZD values of obstacle free cases
are reached.
Flat terrain. The dispersion takes place within an area of uniform buildings. The height of the buildings is 1 Lei (for instantaneous release) or 11 Lee (for continuous release). The lateral measurements of the buildings elements amount to 1 Lei or 11 Lee. The distance from each other is 2 Lei or 21 Lee, respectively.

Flat terrain. The dispersion takes place within an area of uniform buildings. The height of the buildings is 1 Lei (for instantaneous release) or 11 Lee (for continuous release). The lateral measurements of the buildings elements amount to 1 Lei or 11 Lee. The distance from each other is 2,5 Lei or 27 Lee, respectively.

Flat terrain. The dispersion takes place within an area of uniform buildings. The height of the buildings is 1 Lei (for instantaneous release) or 11 Lee (for continuous release). The lateral measurements of the buildings elements amount to 1 Lei or 11 Lee. The distance from each other is 3 Lei or 32 Lee, respectively.


Flat terrain. The dispersion takes place within an area of uniform buildings. The height of the buildings is 1 Lei (for instantaneous release) or 11 Lee (for continuous release). The lateral measurements of the buildings elements amount to 1 Lei or 11 Lee. The distance from each other is 5 Lei or 53 Lee, respectively.

Flat terrain. The dispersion takes place within an area of uniform buildings. The height of the buildings is 2 Lei (for instantaneous release) or 21 Lee (for continuous release). The lateral measurements of the buildings elements amount to 1 Lei or 11 Lee. The distance from each other is 3 Lei or 32 Lee, respectively.

Flat terrain. The dispersion takes places within an area of uniform buildings. The height of the buildings is 2 Lei (for instantaneous release) or 21 Lee (for continuous release). The lateral measurements of the building elements amount to 1 Lei or 11 Lee. The distance from each other is 4 Lei or 43 Lee, respectively.

| Dispersion area type | Delta Xmean [m] | Delta Xworst [m] | Delta tmean [s] | Delta tworst [s] |
| I | 36 Lei | 55 Lei | 65 Tei | 90 Tei |
| II | 50 Lei | 60 Lei | 95 Tei | 105 Tei |
| III | 65 Lei | 75 Lei | 160 Tei | 175 Tei |
| IV | 14 Lei | 19 Lei | 53 Tei | 59 Tei |
| V | 15 Lei | 20 Lei | 50 Tei | 55 Tei |
| VI | 28 Lei | 40 Lei | 60 Tei | 100 Tei |
| VII | 30 Lei | 48 Lei | 75 Tei | 120 Tei |
| VIII | 13 Lei | 16 Lei | 40 Tei | 44 Tei |
| IX | 15 Lei | 20 Lei | 33 Tei | 40 Tei |
| X | 30 Lei | 37 Lei | 80 Tei | 100 Tei |
| XI | 28 Lei | 35 Lei | 70 Tei | 90 Tei |
| XII | 27 Lei | 37 Lei | 50 Tei | 70 Tei |
| XIII | 31 Lei | 37 Lei | 85 Tei | 100 Tei |
| XIV | 30 Lei | 36 Lei | 80 Tei | 95 Tei |
| XV | 27 Lei | 33 Lei | 75 Tei | 90 Tei |
| XVI | 23 Lei | 30 Lei | 60 Tei | 80 Tei |
| XVII | 23 Lei | 31 Lei | 70 Tei | 95 Tei |
| XVIII | 25 Lei | 31 Lei | 65 Tei | 80 Tei |
| XIX | 19 Lei | 24 Lei | 40 Tei | 50 Tei |
| XX | 20 Lei | 24 Lei | 40 Tei | 50 Tei |
| XXI | 22 Lei | 28 Lei | 40 Tei | 50 Tei |
| XXII | 12 Lei | 18 Lei | 25 Tei | 35 Tei |
| XIII | 23 Lei | 29 Lei | 40 Tei | 50 Tei |
| XIV | 19 Lei | 26 Lei | 40 Tei | 45 Tei |
| XV | 20 Lei | 29 Lei | 45 Tei | 50 Tei |
| Dispersion area type | Delta Xmean [m] | Delta Xworst [m] |
| I | 240 Lee | 296 Lee |
| II | 280 Lee | 400 Lee |
| III | 650 Lee | 700 Lee |
| IV | 90 Lee | 122 Lee |
| V | 112 Lee | 130 Lee |
| XI | 149 Lee | 182 Lee |
| XII | 134 Lee | 174 Lee |
| XIII | 102 Lee | 126 Lee |
| IX | 80 Lee | 108 Lee |
| X | 320 Lee | 435 Lee |
| XI | 265 Lee | 300 Lee |
| XII | 245 Lee | 325 Lee |
| XIII | 365 Lee | 490 Lee |
| XIV | 340 Lee | 390 Lee |
| XV | 270 Lee | 370 Lee |
| XVI | 275 Lee | 320 Lee |
| XVII | 245 Lee | 300 Lee |
| XVIII | 215 Lee | 250 Lee |
| XIX | 75 Lee | 118 Lee |
| XX | 105 Lee | 180 Lee |
| XXI | 128 Lee | 185 Lee |
| XXII | 57 Lee | 75 Lee |
| XXIII | 95 Lee | 150 Lee |
| XIV | 90 Lee | 130 Lee |
| XV | 128 Lee | 160 Lee |
* UZD (untere Zünddistanz) = lower flammability distance
© 1981-2010 Petersen & Kade, all rights reserved