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Computers & Geosciences 29 (2003) 961–969
SHEARCALC—a computer program for the calculation ofvolume change and mass transfer in a ductile shear zone$
Robert Sturm*
Institute of Physics and Biophysics, University of Salzburg, Hellbrunnerstrasse 34, A-5020 Salzburg, Austria
Received 1 November 2001; received in revised form 11 April 2003; accepted 16 April 2003
Abstract
SHEARCALC was created to automate mass balance calculations in an alteration zone. The program can be most
successfully applied to ductile shear zones, where an undeformed wall rock is transformed into a fine-grained mylonite
via several protomylonitic stages. The program was written in Visual Basic 6.0 and offers numerous features typical for
Windowst applications to increase the user friendliness. SHEARCALC consists of an input part for entering sample
names, specific weights and chemical data of the investigated rocks as well as for selecting immobile elements and
scaling factors for an appropriate display of the data in the isocon diagram. In the calculation part, the slope of the
isocon and related volume changes between two specific stages of alteration are computed. Additionally, gains and
losses of the main elements during deformation are expressed by respective mass transfer equations. As a special
feature, SHEARCALC contains an extensive diagram section, where the user can select between three chart types.
Besides the classical isocon diagram, mass changes of elements are also displayed in specific two- or three-dimensional
bar charts. Element behaviour along a transsect through the shear zone is documented by two- or three-dimensional
profile graphs. SHEARCALC is a stand-alone application adapted to modern Windowst operating systems and
therefore differs from many available programs in the geoscience which only run in DOS mode.
r 2003 Elsevier Ltd. All rights reserved.
Keywords: Shear zone; Mass balance; Windowst; Visual Basic; Isocon diagram
1. Introduction
Shear zones are outstanding examples of concentrated
deformation caused by the displacement of two adjacent
lithological blocks in the Earth’s crust. If imposed strain
rates are mainly accommodated by ductile processes,
shear zones are characterized by the development of
mylonites from unaltered wall rocks over scales of
centimetres to several 100m (e.g. White et al., 1980).
Due to their often very compact size, ductile shear zones
offer an excellent possibility to study the metamorphic
evolution as well as mechanical and chemical changes
along a predefined transsect of increasing deformation.
Recent investigations of these zones mainly include
questions concerning element mobility and related
volume changes during shearing and alteration processes
(e.g. O’Hara and Blackburn, 1989; Selverstone et al.,
1991; Simpson and de Paor, 1993; Ring, 1996; Hippertt,
1998; Yang et al., 1998). Based upon numerous
publications (see Selverstone et al., 1991 and references
cited therein), mylonitization may happen in the
following three ways (Fig. 1): (1) In ductile shear zones
marked by simple shear and the lack of metamorphic
fluids, mass transfer and volume change during defor-
mation may be regarded as almost negligible (isovolu-
metric shear zones). (2) If plane strain is combined with
transpression and affected rocks are infiltrated by
high amounts of metamorphic fluids, mylonitization
is accompanied by mass depletion and volume loss.
(3) In contrast, a combination of plain strain with
transtension may cause mass supply and volume gain
ARTICLE IN PRESS
$Code available from http://www.iamg.org/CGEditor.
index.htm
*Tel.: +43-662-8044-5709; fax: +43-662-8044-150.
E-mail address: [email protected] (R. Sturm).
0098-3004/03/$ - see front matter r 2003 Elsevier Ltd. All rights reserved.
doi:10.1016/S0098-3004(03)00093-1
within the shear zone (e.g. formation of en echelon
veins). The quantitative description of volume gains
and losses during alteration processes has been intro-
duced in detail by Gresens (1967). A simple graphical
solution of Gresens’ mass transfer equation has been
described by Grant (1986). The results of both publica-
tions form the basis of the computer program presented
in this study.
Available computer programs concerning shear zones
mainly deal with the calculation of shear stress (Fares,
2000) or shear sense indicators (Zhang and Bjornerud,
1995; Jezek et al., 1999). The programs StrainCalculator
and GeoFryPlots by Rod Holcombe (University of
Queensland http://www.earthsiences.uq.edu.au/Brodh/
software) can also be assigned to this group. Computa-
tion of mass balances is limited to the Macintosh
program Mac Gresens (Potdevin, 1993), so far, while a
few other programs simulate comparable alterations in
the pedosphere due to weathering processes (e.g. Biddle
et al., 1998).
ARTICLE IN PRESS
Fig. 1. Types of mass transfer and volume change in ductile shear zones. Whereas ideal simple shear zones normally do not show any
mass transfer and volume change, subsimple convergent shear zones are characterized by an efflux of mass and respective volume loss.
Subsimple divergent shear zones provide a mass influx with related volume gain.
R. Sturm / Computers & Geosciences 29 (2003) 961–969962
The present paper introduces a new computer
program, termed SHEARCALC (version 1.0), for a
comprehensive analysis of geochemical data obtained
from rocks within a ductile shear zone. SHEARCALC
exclusively calculates the mass transfer and related
volume changes in ductile shear zones and therefore
should help to overcome the lack of programs dealing
with this specific field. The program has been written
with Microsoftt Visual Basic 6.0 and is largely based on
the register form concept which enables the creation of a
clear and simply understandable structure. Besides an
extensive calculation block, the program offers numer-
ous diagrams for graphical presentation of the results.
The present contribution first describes all the theory
of mass and volume balancing employed in SHEAR-
CALC, and then explains the attributes and application
of the program.
2. Theoretical background
2.1. Formulation of mass transfer during alteration
processes
Gresens (1967) found a method for the analysis of
changes in volume and concentrations during an
alteration process, which has been applied in many
studies of hydrothermal and upper-grade metamorphic
alteration. Concerning an alteration of A to B; mass
transfer of each element i can be expressed by the
following basic formula:
Xi ¼ fVgB
gACB
i � CAi
� �a: ð1Þ
CAi and CB
i describe the concentrations of component
i in sample A and B; gA and gB are the respective specific
gravities, fv is the volume factor, and a denotes the
reference mass of the original sample (e.g. 100 g).
Equation (1) forms the basis of Gresens’ composition–
volume diagrams (Gresens, 1967; Fig. 3), in which for
each component i the relation between Xi and a set of
arbitrary values of fv is shown. Where the resulting lines
for one or more components intersect Xi ¼ 0; the
respective abscissa value for fv is taken as the volume
factor of alteration. After determination of fv; relativegains and losses of mobile elements can be directly read
from the graph.
Grant (1986) introduced a more effective graphical
method by applying Eq. (1). Instead of a volume ratio fv;the author considered a ratio of equivalent masses after
ðMBÞ and before alteration ðMAÞ; expressed by the
following simple formula:
MB
MA¼
VBgB
VAgA¼ fV
gB
gA: ð2Þ
Changes in mass with respect to the original rock
ðMAÞ can be determined for each component i according
to the equation
MBi ¼ MA
i þ DMi; ð3Þ
where DMi denotes the mass change of component i: Totransform mass units into concentration units, Eq. (3) is
normalized against MA and subsequently multiplied by
ðMA=MBÞ:
MBi
MB¼
MAMBi
MBMA¼
MA
MB
MAi
MAþDMi
MA
� �: ð4Þ
Eq. (4) can now be written with concentration units in
the following way:
CBi ¼
MA
MBðCA
i þ DCiÞ: ð5Þ
Eq. (5) represents the basic expression of Grant’s
approach and is used to define the so-called ‘isocon’ by
plotting the analytical data of CBi against CA
i and
drawing a line through those (immobile) components
characterized by DCi ¼ 0: The resulting line runs
through the origin of the graph and has the slope
ðMA=MBÞ: The obtained reference line offers an
excellent way to calculate relative gains and losses of
mobile components by simply checking the displace-
ments of respective data points from the isocon.
Mathematically this can be best determined by dividing
both sides of Eq. (5) by CAi :
CBi
CAi
¼MA
MB
CAi
CAi
þDCi
CAi
� �: ð6Þ
Rearrangement of Eq. (6) results in the following
expression:
DCi
CAi
¼MB
MA
� �CB
i
CAi
� �� 1: ð7Þ
Determination of volume changes during the altera-
tion process can be carried out by simply rearranging
Eq. (2) to
VB
VA¼
MB
MA
� �gA
gB
� �: ð8Þ
VB=VAo1 indicates volume loss, VB=VA > 1 volume
gain. If VB=VA ¼ 1; alteration has taken place iso-
volumetrically. The quantity of volume change can be
easily checked from Eq. (8) by setting VA ¼ 1 (or 100%)
and calculating the resulting value of VB:
2.2. Calculation of the isocon using linear regression
analysis
The slope MA=MB of the isocon is determined by
plotting oxide and element concentrations of the altered
rock against those of the wall rock and by fitting a
regression line through the data points representing
immobile elements. From a mathematical point of view,
ARTICLE IN PRESSR. Sturm / Computers & Geosciences 29 (2003) 961–969 963
MA=MB can be now expressed as follows (least-squares
method):
MA
MB¼
Pi CA
i CBiP
iðCAi Þ
2: ð9Þ
The goodness-of-fit can be best expressed by the
parameter r2; where r denotes the correlation coefficient
of the plotted concentration data:
r2 ¼P
iðCB0
i � CBðmÞÞ2PiðC
Bi � CBðmÞÞ2
: ð10Þ
In Eq. (10), CiB0
is the respective concentration point
of the immobile component i on the regression line,
CBðmÞ is the mean of all immobile component concen-
trations of B: Another parameter describing the quality
of the fitted regression line is the standard error of
estimation for the slope MA=MB which is represented by
the following equation:
MA
MBðerrÞ ¼
ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiP
i CBi �
MA
MBCA
i
� �2
ðn � 2ÞP
iðCAi � CAðmÞÞ2
vuuuut : ð11Þ
The program algorithm of SHEARCALC is based on
the equations presented. Design and use of the program
will be described in detail in the next section.
3. Program description
3.1. Data processing
SHEARCALC computes the mass balance and
volume change between two rocks characterized by
different grades of alteration. The program can be best
applied to ductile shear zones, where a wall rock is
transformed into a high-grade mylonite by passing
through several protomylonitic stages. SHEARCALC
also offers the possibility to calculate losses or gains of
mass and volume between the intermediate stages of
alteration. Results of the calculations are presented on
specific forms and can be printed out optionally.
Additionally, the program includes an extensive diagram
section for a convenient graphical display of the results.
SHEARCALC was designed and programmed in Visual
Basic 6.0. This computer language allows to create very
user-friendly applications with the typical features of a
Windowst program (menu bar, symbol bar, etc.).
Although the design of SHEARCALC shows some
specificities like horizontal and vertical register bars, all
users familiar to any Windowst application should be
able to navigate successfully through the respective
forms, at once. The navigation is realized by simply
clicking on an element of the register bars or a button in
the symbol bar. Each active element or button is
characterized by a change of the mouse pointer into a
pointing hand symbol. SHEARCALC has the advan-
tage to run as a stand-alone application within the
Windowst operating system (Version 98 or 2000).
Many scientific programs written in other languages
than Visual Basic 6.0 (e.g. QuickBasic, Fortran,
TurboPascal, C) mainly run in the DOS environment
and therefore partly cause higher operating times or
conflicts with the Windowst operating system.
In general, the presented program can be subdivided
into six main parts, to which the user can navigate by
simply clicking on the respective elements of the vertical
register and the uppermost button of each symbol bar:
1. ENTRANCE: From here, the user can navigate to
the main parts of the program or leave SHEAR-
CALC, again. In this form, also first steps for a
successful use of the program as well as interesting
links in the world wide web are available (Fig. 2A).
2. INPUT: In this part of the program, sample names,
specific weights and chemical data (main and trace
element concentrations; mean values and standard
deviations SD) of an undeformed wall rock as well as
five different stages of deformation labelled with
mylonite 1–5 can be entered (Fig. 2B).
3. IMMOBILE ELEMENTS/SCALING FACTORS:
This part of SHEARCALC allows the selection of
elements considered as immobile during the process of
deformation (Fig. 2C). The input of scaling factors is
necessary for a convenient display of all selected
elements in the isocon diagram (Grant, 1986; Fig. 2D).
4. ISOCON: In this part, the isocons are calculated by
linear regression analysis for different transforma-
tions (e.g. transformation of wall rock into mylonite
5, etc.). The standard error of the isocon slopes,
goodness-of-fit (indicated by r2) as well as type and
relative quantity of volume change are computed
additionally (Fig. 2E).
5. MASS BALANCE: This part of SHEARCALC
provides the mass balance equations (Gresens, 1967)
for transitions between wall rock and mylonites as well
as between different mylonitic stages (Fig. 2F).
6. DIAGRAMS: In this part, the user can select
between three diagram types for a graphical dis-
play of the chemical data and calculation results
(Fig. 2G): (a) isocon diagrams; (b) bar charts to
visualize relative gains and losses of elements during
deformation; (c) line charts showing the behaviour of
elements throughout the zone of alteration.
Except for the ENTRANCE part, each form of
SHEARCALC contains a vertical register bar on the
right side for navigation to the main program sections
and a symbol bar on the left side for specific actions
useful in a Windowst program. As documented above,
within SHEARCALC the forms for data input and data
output are clearly separated. Therefore, the user is not
ARTICLE IN PRESSR. Sturm / Computers & Geosciences 29 (2003) 961–969964
able to manipulate any of the calculated results. After
each change of the input data, calculations have to be
carried out from the beginning and are not recalculated
automatically.
In the present contribution the program was tested on
chemical data from a shear zone described in detail by
Sturm and Steyrer (2003). The deformation zone is
located in the western part of the Tauern Window
(Eastern Alps, Austria) and has been formed under
medium- to deep-crustal P2T conditions. In general,
besides the wall rock (sample AS 14/92) five mylonitic
stages (samples 815A–E) could be distinguished. From
each deformation stage at least five samples have been
analysed chemically to recognize possible inhomogene-
ities in composition. Input data are listed in Table 1,
while selected results of calculation are shown in Figs. 2
and 3.
3.2. Graphics
SHEARCALC contains an extensive DIAGRAM
section for an appropriate visualization of input data
and results from diverse calculations. While chemical
data of the INPUT forms can be plotted in profiles
documenting chemical changes along a predefined
transsect, isocon diagrams help to describe the mobility
of certain elements within the investigated alteration or
shear zone. Mass transfers of the main elements between
two deformational stages are also presented graphically
in specific bar charts (Fig. 2G).
3.2.1. Isocon diagrams
Clicking on the isocon diagram button of the
DIAGRAM form opens a new window containing
several command buttons in the upper right corner
and an empty drawing area. After activation of the
DRAW button by a mouse click or with the TAB and
RETURN keys, the isocon diagram illustrating element
mobilities between two deformational stages of the shear
zone is drawn (Fig. 3A). Only those elements selected in
the SCALING form are plotted, and concentrations
(and standard deviations) are increased or decreased by
the respective scaling factors. The isocon, line of
constant mass, and line of constant volume are
ARTICLE IN PRESS
Table 1
Geochemical data from deep-crustal shear zone of western Tauern Window (Austria; Sturm and Steyrer, 2003)
Sample AS 14/92 815E 815D 815C 815B 815A
Rock Wall rock Mylonite 1 Mylonite 2 Mylonite 3 Mylonite 4 Mylonite 5
Conc. SD Conc. SD Conc. SD Conc. SD Conc. SD Conc. SD
Main elements (wt%)
SiO2 63.90 1.92 62.00 2.85 58.30 3.09 51.00 3.47 46.20 3.28 40.80 3.39
TiO2 0.66 0.02 0.76 0.03 0.82 0.04 0.83 0.06 0.72 0.05 0.80 0.07
Al2O3 17.00 0.51 16.60 0.76 18.50 0.98 19.00 1.29 20.60 1.46 19.80 1.64
Fe2O3 5.35 0.16 8.56 0.39 9.27 0.49 12.00 0.82 15.90 1.13 20.40 1.69
MgO 1.83 0.05 3.06 0.14 3.46 0.18 5.28 0.36 6.24 0.44 6.55 0.54
MnO 0.10 0.00 0.11 0.01 0.11 0.01 0.13 0.01 0.16 0.01 0.24 0.02
CaO 4.90 0.15 2.34 0.11 2.14 0.11 3.21 0.22 2.78 0.20 2.72 0.23
K2O 2.08 0.06 2.72 0.13 2.96 0.16 3.20 0.22 4.00 0.28 4.24 0.35
Na2O 4.00 0.12 2.13 0.10 2.20 0.12 3.06 0.21 1.80 0.13 0.84 0.07
P2O5 0.18 0.01 0.19 0.01 0.14 0.01 0.17 0.01 0.16 0.01 0.22 0.02
LOI 0.75 0.02 1.60 0.07 1.80 0.10 1.70 0.12 2.20 0.16 2.85 0.24
Total 100.75 100.07 99.70 99.58 100.76 99.46
Trace elements (ppm)
Nb 17 0.68 18 0.56 17 0.90 19 1.29 15 1.07 13 1.08
Zr 181 7.24 181 8.33 189 10.02 184 12.51 190 13.49 216 17.93
Y 11 0.34 18 0.64 22 1.17 29 1.97 17 1.21 17 1.41
Sr 315 12.60 164 7.54 174 9.22 163 11.08 110 7.81 98 8.13
Rb 88 3.52 97 4.46 103 5.46 102 6.94 148 10.51 164 13.61
Cr 11 0.44 18 0.83 14 0.74 12 0.82 11 0.78 10 0.83
Ni 6 0.24 7 0.32 10 0.53 13 0.88 8 0.57 8 0.66
Ba 442 17.68 513 23.60 380 20.14 240 16.32 350 24.85 518 42.99
Hf 4.8 0.19 5 0.23 4.9 0.26 5.4 0.37 4.5 0.32 4.2 0.35
Specific weight (g/cm3) 2.87 2.94 3.03 3.08 3.14 3.20
Data were used to test SHEARCALC. Grade of deformation is increased from Mylonite 1 to Mylonite 5.
R. Sturm / Computers & Geosciences 29 (2003) 961–969 965
displayed with different signatures (solid, dashed, and
dotted). Abscissa and ordinate of the diagram are
labelled with the rocks, whose element concentrations
and standard deviations are plotted in the graph. Scaling
of both x- and y-axis uniformly ranges from 0 to
50wt%. BACK and FORWARD buttons will navigate
ARTICLE IN PRESS
Fig. 2. (A–G) Entrance, input and calculation forms of SHEARCALC. Except for the ENTRANCE form, all forms are characterized
by their uniform organization with horizontal and vertical registers as well as a symbol bar on left side.
R. Sturm / Computers & Geosciences 29 (2003) 961–969966
ARTICLE IN PRESS
Fig. 3. Graphs produced by SHEARCALC: (A) isocon diagram (data points with SD rectangles), (B) two-dimensional mass transfer
diagram, (C) three-dimensional mass transfer diagram with autoscaling, (D) two-dimensional profile diagram, (E) three-dimensional
profile diagram with autoscaling.
R. Sturm / Computers & Geosciences 29 (2003) 961–969 967
through all possible isocon diagrams (up to 9), whereas
with the PRINT button a high-quality print of the graph
is produced.
3.2.2. Mass transfer diagrams
Activation of the medium button in the DIAGRAM
form opens a window that differs from the respective
isocon diagram window only in some details. Besides the
DRAW button, three input fields have been generated
which allow the determination of a minimum and
maximum ordinate value as well as the selection of
the distance between the major tics. After clicking the
DRAW button, a two-dimensional bar chart with
the specific properties entered above will be generated
(Fig. 3B). The topic of the diagram describes the
transition for which the mass balance equation was
calculated. As a further characteristic, respective results
can be also drawn in a three-dimensional graph. This is
realized by simply clicking on the 3D-GRAPH button.
After appearance of a new window containing a default
diagram, activation of the DRAW button generates the
desired chart (Fig. 3C). In each three-dimensional graph
five transition types are displayed. Scaling of the y-axis is
done automatically. The window of two-dimensional
diagrams can be activated again by clicking on the 2D-
GRAPH button.
3.2.3. Chemical profiles
As an additional feature of SHEARCALC, the user
can draw chemical profiles through the alteration zone.
This is realized by clicking the third button of the
DIAGRAM form. A window very similar to that of the
mass transfer diagram is opened. In the data fields, the
user can enter minimum and maximum values of the y-
axis as well as the distance between two major tics. After
clicking on the DRAW button, the desired graph is
displayed (Fig. 3D). For a better overview, each graph
only contains the profiles of five elements which are
listed in the legend on the right side. With the 3D-
GRAPH button a three-dimensional line chart can be
created, again. Similar to the mass transfer graph,
scaling of the ordinate is carried out automatically
(Fig. 3E).
3.3. Data output
By using the PRINT button, respective input data,
results of calculations, and graphs can be printed out,
optionally. Within the input and calculation forms, a
small menu is opened after clicking on the PRINT
command, where the user can select between printing the
activated form or a summary of computation containing
all raw data entered into the input section, the elements
assumed as immobile, the calculated isocons, the good-
ness-of-fit, the estimated volume changes, and the
related mass balance equations. Using the PRINT
button in the DIAGRAM forms results in printing out
the activated graph on a single sheet of paper.
Manipulation of a diagram is not possible at the
moment, but will be implemented in a future version
of SHEARCALC.
4. System requirements and availability of the program
SHEARCALC was programmed with the latest
version of MicrosoftTM Visual Basic. To take advantage
of the graphical layout of the program, a Pentium-IIt
computer with an SVGA graphic card is highly
recommended. Further, a newer version of Windowst
(98 or 2000) must be installed to guarantee a trouble-free
execution of the program. For execution of the program,
VBRUN.DLL must be included in the Windowst
system folder. Printing out of the charts should be done
either with a high-resolution inkjet printer or a laser
printer. Program files can be directly obtained from the
author via E-mail, or downloaded from the IAMG
server.
Acknowledgements
The author thanks the two anonymous reviewers, who
have helped to improve the paper significantly.
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