Mediterranean Archaeology and Archaeometry, Vol. 18, No 1, (2018), pp. 221-236
Copyright © 2018 MAA
Open Access. Printed in Greece. All rights reserved.
DOI: 10.5281/zenodo.1165360
INTEGRATED DYNAMIC AND THERMOGRAPHY
INVESTIGATION OF MALLORCA CATHEDRAL
Ahmed Elyamani1, Oriol Caselles2, Pere Roca2 and Jaime Clapes2
1Archaeological
2Department
Conservation Department, Cairo University, Giza, Egypt
of Civil and Environmental Engineering, Technical University of Catalonia, Barcelona, Spain
Received: 10/09/2017
Accepted: 31/01/2018
Corresponding author: Ahmed Elyamani (a_elyamani@cu.edu.eg)
ABSTRACT
An integrated investigation of engineering archaeometry was carried out using dynamic identification,
dynamic monitoring and Infra-Red (IR) thermography for the study of the dynamic behavior of Mallorca
cathedral in Spain. The cathedral is a large historical masonry structure built during 14-16th c. Dynamic
identification and monitoring allowed the capturing of eight natural frequencies of the cathedral. IR
thermography was used as a complementary inspection technique in the context of a continuous monitoring.
Usually, IR thermography is used punctually for the inspection of a part of an inspected structure. Here an
alternative was tried as the IR camera was installed for two two-weeks periods in the winter and in the
summer of 2011 to monitor the stone surface temperature of a large portion of the cathedral. The correlation
between the cathedral natural frequencies and the stone surface temperature of some selected structural
elements was investigated and compared with the correlation with the external and the internal
temperatures. It was found that the correlation with stone surface temperature was lower than that with
external temperature. The study allowed a better understanding of the influence of temperature changes on
the structure’s dynamic behavior.
KEYWORDS: Mallorca Cathedral, Historical Structures, In-situ Investigation, Dynamic Identification, Dynamic Monitoring, IR Thermography, Air Temperature, Stone Temperature
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1.
A. ELYAMANI et al.
INTRODUCTION
Historical structures are very important assets of
the world heritage as cultural resources involving
important artistic, spiritual, technical and scientific
merits. They contribute to the identity of cultures
and countries and provide valuable documents on
the great achievements from the past. Moreover,
they represent important economic resources. For
these reasons and many others, modern societies
allocate great technical and economical effort to the
conservation of their architectural heritage. European researchers, in particular, have carried out a
number of research projects on the subject (PERPETUATE, 2010-2012, SEVERES, 2010-2012, PROHITECH, 2004-2008, EU-INDIA, 2004-2006, RISKUE, 2001-2004, CHIME, 2000-2003).
In fact, the preservation of the architectural heritage faces significant challenges ranging from the difficulty in understanding the historical construction
materials to the complexity of possible actions influencing on it. Due to these difficulties, often faced
when assessing the structural safety of a historic
structure, the assessment of heritage structures requires combining different approaches such as historical investigation, inspection, experiments, static
monitoring, dynamic monitoring and structural
analysis. The aim is to respect the authenticity of the
historic structure, to the extent possible, by designing an efficient solution which, while attaining the
required safety level, minimizes the impact in terms
of material and structural alteration. In the study
here presented, dynamic identification, dynamic
monitoring and Infra-Red (IR) thermography were
employed for studying the dynamic behavior of
Mallorca cathedral, one of the largest worldwide
masonry historical structures, and its dependency on
external temperature, internal temperature and stone
surface temperature.
Two different but interconnected activities, namely dynamic identification and dynamic monitoring,
can be envisaged for the study of the dynamic response of historical structures. While dynamic identification is based on punctual measurements of the
dynamic response by means of tests performed in a
discrete way, dynamic monitoring involves the continuous measurement of the dynamic properties.
Dynamic identification is carried out to obtain information on the global dynamic behavior of the
structure, including natural frequencies, mode
shapes and damping coefficients. It is also an efficient tool to validate and update structural numerical models by comparing experimental and numerical natural frequencies and mode shapes (Elyamani
and Roca, 2018a,b). Some of the early applications of
dynamic identification in studying historic struc-
tures can be found in (Chiostrini et al., 1992; Erdik et
al., 1993; Modena et al., 1997). For recent applications, the reader is referred to (Diaferio et al., 2015;
Foti et al., 2014; Ceroni et al., 2014; Cagnan et al.,
2015; Votsis et al., 2015; Votsis et al., 2012).
Dynamic monitoring can be carried out to confirm
the obtained information from the dynamic identification. Additionally, it aims at studying the evolution of modal parameters in time, studying the influence of environmental climatic effects (temperature,
humidity, etc.) on the dynamic parameters and capturing the dynamic response in the occasion of possible seismic events, among other possible purposes
(Elyamani and Roca, 2018a,b). Some recent applications have been presented by (Masciotta et al., 2016;
Basto et al., 2016; Lorenzoni et al., 2013; Rivera et al.,
2008; Cabboi et al., 2014).
Most materials absorb Infrared Radiation (IR)
over a wide range of wavelengths which results in
an increase in their temperature. When an object has
a temperature greater than absolute zero it emits IR
energy. IR thermography is a nondestructive inspection technique which converts the emitted IR radiation pattern into a visual image by the usage of an IR
camera. An IR camera measures, calculates and displays the emitted IR radiation from an object (Clark
et al., 2003).
IR thermography has been applied to several emblematic historical structures for inspection purposes. For instance, the IR thermography was used extensively in the inspection activities carried out on
the church of Nativity in Bethlehem (Faella et al.,
2012). The IR thermography showed: 1) moisture
problems due to rainwater seepage and re-climbing
moisture presence in several masonry walls; 2) the
plugging of some openings; 3) nearly homogenous
materials used in the roof except one area in which
different materials were used; and 4) great seepages
of rainwater in the narthex roof caused by the lack of
an efficient waste disposal system for drainage. Binda et al. (Binda et al., 2011) used IR thermography as
one of the inspection techniques applied to the Spanish Fortress damaged by L’Aquila earthquake. Because the masonry was hidden by thick plaster, the
IR thermography was used to reveal its texture,
which helped in identifying the most representative
areas where to execute minor destructive tests like
flat-jack. Tavukçuoğlu et al. (2010) used the IR thermography in the inspection of a 16th century historical mosque. The aim was to discover the activeness
of observed structural cracks. Other studies involving the use of thermography in ancient structures
can be found in (Jo and Lee, 2014; Alves et al., 2014;
Bagavathiappan et al., 2013; Martinez et al., 2013).
This research was carried out within the research
project NIKER (NIKER, 2010-2012) aimed at investi-
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INTEGRATED DYNAMIC AND THERMOGRAPHY INVESTIGATION OF MALLORCA CATHEDRAL
gating the effects of earthquakes on historical constructions via extensive experimental and numerical
studies applied to several case studies. Mallorca cathedral was chosen as one of the selected case studies. A comprehensive review on the restoration of
the cathedral is given in Elyamani and Roca (2018c).
The experimental investigation activities employed for the study of the cathedral included Ambient Vibration Testing (AVT) and dynamic monitoring. An IR thermography was used as a complementary system for the measurement of temperature.
Usually, the IR thermography is used punctually for
inspecting a certain part of a structure. Here, an alternative application was tried. The IR camera was
used to continuously monitor the temperature during two two-weeks periods within summer and winter of 2011. This allowed a detailed investigation of
the correlation between the natural frequencies of
the cathedral and the stone surface temperature of
different structural elements of the cathedral like
columns, vaults and arches.
223
Mallorca cathedral is a Cultural Heritage of National Interest in Spain since 1931 (Figs.1 and 2). It is
located in the city of Palma, in Mallorca Island.
When compared with other worldwide Gothic cathedrals, it is found that its piers show an unusually
large slenderness ratio, while its main nave span is
the second longest span among Gothic cathedrals
after Girona cathedral. Its main nave is among the
highest ones after those of Beauvais and Milan cathedrals.
The construction started in the beginning of the
14th century and continued to the beginning of the
17th century. The first built part was the Trinity
Chapel (part I in Figure 3) in year 1311. About 60
years later the Royal Chapel (part II in Figure 3) was
finished. It was then decided to modify the design
from that of a single nave building to a three-nave
one. No documented justifications behind this decision were revealed by any historical research carried
so far about the cathedral construction. The imposing main large nave and the west facade (part III in
Figure 3) were completed by the year 1601.
2. MALLORCA CATHEDRAL
Figure 1. Mallorca Cathedral from outside: apse area (left), south façade (centre) and main façade (right).
Regarding the geometrical configuration of the cathedral (Figure 3), it is found that the main nave has
a length of 77 m distributed over eight bays and the
width covered by the naves is 35.3 m. The lateral
nave and the central nave spans are 8.75 m and 17.8
m, respectively. The lateral naves are covered by
pointed vaults of simple square plan. The central
nave is covered by vaults of double square plan. This
scheme is repeated in all the bays of the naves except
in the 5th one (from the choir), due to the presence of
lateral doors. In this bay, the longitudinal span of the
vaults is slightly longer. The height reached by the
vaults at their highest point (the key of the transverse arches) is about 44 m. The cathedral is also
unique in being the Gothic cathedral with the highest lateral naves (29.4 m). All of the octagonal columns have a circumscribed diameter of 1.7 m except
those of the first three bays from the choir that have
a slightly lesser value of 1.6 m. More information on
the cathedral can be found at (Caselles et al., 2012;
Elyamani et al., 2017a; Gonzalez et al., 2008; Elyamani et al., 2017b; Pela et al., 2014; Elyamani, 2015; Caselles et al., 2015; Elyamani et al., 2012; Roca et al.,
2013).
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A. ELYAMANI et al.
(a)
(b)
(c)
(d)
Figure 2. Internal views of Mallorca cathedral: (a) view of the choir, central nave and south lateral nave; (b) view of the
west façade and north nave showing the slenderness of columns and the upper and lower clerestory walls; (c) view of
the central nave from the choir; and (d) central nave vaults .
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I
II
225
III
Figure 3.Mallorca cathedral: (a) plan and (b) longitudinal section [48].
2. DYNAMIC INVESTIGATION OF THE
CATHEDRAL
2.1 Ambient vibration testing (AVT)
The objective of AVT was to identify the natural
frequencies, mode shapes and damping ratios of the
cathedral. The natural frequencies and modes shapes
were used to update the numerical model of the cathedral which was then used in the seismic analysis
of it (Elyamani et al., 2017a). A brief about AVT is
given here and full details can be consulted at (Elyamani et al., 2017b; Elyamani, 2015).
The tests configuration was based on a preliminary modal analysis carried out using an initial FE
model of the cathedral. It was noticed that only the
first and the second modes were global ones with
considerable mass participation and characterized
by predominant movement of the main and lateral
naves of the cathedral. Consequently, the used accelerometers were organized in different setups so that
capturing these two modes would be achievable.
Three tri-axial force balance accelerometers were
used in AVT and the sampling rate was 100 samples
per second.
The obtained signals during AVT were processed
for dynamic identification using MACEC software
(MACEC, 2011). Four different methods were employed: the Frequency Domain Decomposition
(FDD) (Brincker et al., 2001); reference-based covariance-driven Stochastic Subspace Identification (SSIcov/ref) (Peeters and De Roeck, 1999); referencebased data-driven Stochastic Subspace Identification
(SSI-data/ref) (Peetres and De Roeck, 1999) and
poly-reference Least Squares Complex Frequency
domain identification (pLSCF) (Peetres and Van der
Auweraer, 2005). Eight modes were identified. The
natural frequencies of all of them were satisfactory
identified (Table 1), whereas, the mode shapes and
the damping ratios of only three of them were satisfactory identified.
Table 1. Identified natural frequencies (Hz) using different methods.
Identification
method
FDD
SSI-cov/ref
SSI-data/ref
pLSCF
1
1.143
1.162
1.166
1.145
2
1.431
1.433
1.445
1.430
3
1.503
1.511
1.514
1.509
Mode ID.
4
5
1.569
1.942
1.576
1.939
1.576
1.942
1.576
1.943
6
2.232
2.214
2.241
2.234
7
2.406
2.421
2.434
2.432
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8
2.649
2.656
2.662
2.666
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2.2 Dynamic monitoring
The use of AVT was followed by a continuous
dynamic monitoring system. A brief is given here
and more details can be referred to at (Elyamani et
al., 2017b; Elyamani, 2015). The system was composed of a digitizer, a Data Acquisition system
(DAQ), a Global Positioning System (GPS) antenna,
an internet router and the three tri-axial accelerometers previously used in the dynamic identification
tests, Figure 4. The system worked properly for two
periods: from 17/12/2010 to 13/9/2011and from
18/5/2012 to 29/12/2012. Within this second period,
the system was interrupted from 30/7/2012 to
4/9/2012. The system was programmed to continu-
ously measure, record, and wirelessly transfer the
records of the accelerations on a 24 h basis. The natural frequencies were determined manually using the
Peak Picking (PP) method four times per day: at 6
a.m. (06:00), 2 p.m. (14:00), 8 p.m. (20:00) and 12 a.m.
(24:00) during the entire monitored periods.
The eight natural frequencies identified from AVT
were identified continuously by the system. The
identified natural frequencies were plotted versus
the time as presented in Figure 5. The gap in the second period corresponds to the dates previously mentioned during which the system was out of service
due to technical problems.
Figure 4.The dynamic system in operation: accelerometer S1, DAQ, router and GPS antenna (left);
accelerometer 145-Station and digitizer (middle); and accelerometer Soil-station (right).
Mode 8
Mode 7
Mode 6
Mode 5
Mode 4
Mode 3
Mode 2
Mode 1
Figure 5. Evolution of the natural frequencies of the cathedral over time.
In the first monitoring period, the cathedral natural frequencies showed an increasing trend that can
be attributed to the raising of the temperature, since
the monitoring started in winter and ended in summer. The contrary was found for the second monitor-
ing period during which a decreasing trend was noticed, also attributed to the temperature variations as
the monitoring started in summer and ended in winter.
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Table 2. Comparing natural frequencies (Hz) from AVT and dynamic monitoring, and amount of changes of the natural
frequencies over the monitoring period.
Mode number
AVT (SSI-cov/ref)
Dynamic monitoring
Coefficient of Variation (CV) (%)
(Max.–Min.)/Max. (%)
1
1.162
1.158
7.1
31.8
2
1.433
1.496
2.57
14.9
3
1.511
1.576
2.49
13.9
4
1.576
1.631
2.29
10.4
5
1.939
1.988
3.51
17.0
6
2.214
2.353
3.48
16.6
7
2.421
2.593
3.74
18.5
8
2.656
2.797
3.18
14.3
Table 3. Correlation coefficients between temperature and cathedral frequencies.
Mode ID.
Regression model
Linear
Quadratic
1
0.197
0.241
2
0.766
0.802
3
0.544
0.544
4
0.834
0.854
5
0.618
0.643
6
0.640
0.660
7
0.602
0.603
8
0.806
0.819
Figure 6. Changes of the natural frequency of mode 4 with external temperature (top) and correlation with external temperature (bottom). Linear and quadratic regression models are in solid and dashed lines, respectively.
It can be observed that modes 2, 3, 4 and 8 showed
curves characterized by more continuous and intensive readings when compared to the curves of the
other modes 1, 5, 6 and 7, that showed less continuity and intensity of readings. In addition, the curves
of modes 2, 3, 4 and 8 showed a lesser scattering in
comparison with the curves of other modes. The increasing and decreasing trends observed over time
were clearer in the case of the continuously detected
modes 2, 3, 4 and 8, whereas no distinguishable
trends were observed for the remaining modes.
The frequencies detected in the dynamic tests were
lesser than the mean values found by the dynamic
monitoring system, Table 2. This difference can be
attributed to the fact that the tests were performed in
winter, whereas the monitoring system covered several summer months. The months from May to July
and also half of the month of September were repeated two times in the entire monitoring period, thus
resulting in an average temperature about 18.4 °C,
whereas in the tests it was about 7.4 °C.
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A. ELYAMANI et al.
Table 2 also reports the changes of the natural frequencies over the whole monitoring period. In terms
of coefficient of variation (CV), the modes 2, 3, 4, and
8 showed the lowest values. These modes were more
centralized and manifested less variability when
compared with the rest of the modes which had
higher CV values. The same note can be stated when
relating the range (maximum–minimum) with the
maximum value as shown in the last row of the table. The Modes 2, 3, 4, and 8 had less variability than
other modes. The very high value of Mode 1 could
be related to the difficulty of detection rather than to
changes in environmental conditions.
The change of the frequencies with temperature
was plotted for the eight detected modes (Figure 6
for mode 4 as an example). It was noticed that the
relation was clearer and the in-phase oscillation was
more evident for modes 2, 4 and 8 than for modes 3,
5, 6 and 7. The frequency variations under changes
of exterior temperature were investigated and both
the correlation and the regression were studied, Figure 6. It can be noticed in Figure 6 that the trend is
not exactly linear. Therefore, both of linear regression and quadratic regression were considered to
investigate into more detail the type of the relation
between temperature and frequencies. The obtained
correlation coefficients are summarized in Table 3.
As can be seen from the comparison among all models, a linear relation between temperature and natural frequencies provided a good approximation. No
significant increase in the coefficients of correlation
was obtained when considering a higher degree
model. The correlation coefficient of the quadratic
model was only slightly higher than that of the line-
ar one. The highest correlation value was around
0.80 to 0.86 for modes 2, 4 and 8, followed by the correlation coefficients ranging from 0.55 to 0.66 for
modes 3, 5, 6, and 7.
3.
THERMOGRAPHIC INVESTIGATION
3.1 Description of the thermographic
monitoring System
An infrared (IR) camera of type “Thermo GEAR
G120” produced by NEC Company was used. Its
main characteristics are: 1) measuring range from 40° C to 500° C with accuracy of ±2°C or ±2% of
reading, whichever is greater; 2) thermal image of
320 pixels (horizontal) X 240 pixels (vertical); 3) spectral range from 8 to 14 μm; 4) frame rate of 60
frames/sec; 5) automatic focusing with focal distance from 10 cm to infinity; and 6) automatic recording of images with interval from 3s to 60 min.
It worked at the same location in two periods: 1)
in the winter of 2011 for 14 days from 27/1 (at 11:15)
to 9/2 (at 23:45), and 2) in the summer of the same
year for 16 days from 28/6 (at 8:16) to 13/7 (at
22:46).
The IR camera position and its coverage area are
shown in Figure 7. As shown, it was located inside
the north pulpit and directed to the arches, the
vaults, the upper clerestory and the columns of the
main nave. This place allowed the IR camera to cover a large portion of the first five bays of the main
nave. The IR camera recorded photos each half an
hour. A sample of the monitoring photos in the
summer and the winter periods is shown in Figure 8.
West
facade
(a)
(b)
(c)
Figure 7. Mallorca cathedral thermography monitoring: (a) the red circle shows the IR camera position; (b) the IR camera during operation (inside the pulpit); and (c) the area covered by the IR camera.
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229
Figure 8. Two examples of the thermography monitoring: 1) summer period on 2nd of July 2011 at 9:46 a.m. (top); and 2)
winter period on 2nd of February 2011 at 13:15 (bottom). Temperature scale in (°C).
3.2 Comparisons between different
temperatures
For each day of the two monitoring periods, four
IR photos were processed at the same times of the
dynamic monitoring data, i.e., at 6 a.m., 2 p.m., 8
p.m. and 12 a.m. Using the software “Inf ReC Analyzer NS9500 Standard” which was provided with
the IR camera, the stone surface temperature was
determined for two samples from the considered
structural elements (the columns, the clerestory
walls, the arches and the vaults) as shown in Figure
9. In the figure also the places of the three temperature sensors used in the summer period are shown.
The stone surface temperature recorded is influenced by the distance from the IR camera, the ambient relative humidity, the ambient temperature and
the stone emissivity. The available geometrical sur-
vey of the cathedral provided the distance from the
IR camera to each of the considered structural elements samples. An average ambient relative humidity and temperature of 65% and 27.9 °c, respectively,
were used for the summer period and 83% and 13.5
°c for the winter period. These approximate values
were estimated from the previous static monitoring
system that worked for five years (from 2003 to 2008)
and showed clearly the repeated cycles experienced
by these parameters. More details about this monitoring are available in (Gonzalez et al., 2008). Regarding, the stone emissivity, the cathedral was built
mainly from limestone which has an emissivity of
0.95 according to the references on the subject
(Gosse, 1986; Adler, 1969).
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A. ELYAMANI et al.
Figure 9. Selected samples from structural elements within the IR camera coverage area: clerestory walls and columns
(top), arches, columns and vaults (bottom). Coverage area hatched in light brown.
Figure 10. Comparison between external, internal and stone surface temperatures in the summer period from 28/6/2011 to
13/7/2011.
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Figure 11. Comparison between external and stone surface temperatures in the winter period from 27/1/2011 to 9/2/2011.
Figure 12. Comparison between external temperatures for the summer and winter periods. The trend lines are also shown.
A comparison was made between the external
temperature (measured from a near meteorological
station), the internal temperature (measured in
summer only using temperature sensors) and the
stone surface temperature of the considered structural elements for the summer period (Figure 10)
and the winter period (Figure 11). It can be seen that
the stone surface temperatures of the different struc-
tural elements were in phase and very near to each
other for the two monitoring periods. For the summer period, the internal and the external temperatures were in phase, whereas, the stone surface temperature was sometimes delayed with respect to the
external and the internal temperatures. In the winter
period, the stone surface temperature was in phase
with the external temperature.
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To explain the reason of the delay of the stone surface temperature in the summer period, a comparison between the external temperature of the summer
and the winter periods is shown in Figure 12. It can
be noticed that an increasing trend was observed
during the summer period, whereas a constant trend
was obtained during winter. It can be assumed that,
in the summer period, the stone was not able to radiate the stored heat as fast as the rapidly increasing
external temperature, therefore producing a delay in
the variation of surface temperature with respect to
the external one. This phenomenon disappeared in
the winter period during which the stone could ra-
diate the heat in phase with the almost constant rate
of change of the external temperature.
3.3 Correlation between natural frequencies and
different temperatures
An acceptable qualitative correlation was found
between the natural frequencies of the cathedral and
the stone temperature changes. Figure 13 shows this
correlation for mode 4 as an example. The stone surface temperature indicated in Figure 13 corresponds
to the average temperature of the columns, the
vaults, the arches and the clerestory walls.
Figure 13. Changes of mode 4 with stone temperature: summer period (top); and winter period (bottom).
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Figure 14. Summer period: comparison between coefficients of correlation of different temperatures with the first eight
modes of the cathedral.
Figure 15. Winter period: comparison between coefficients of correlation of different temperatures with four of the cathedral modes.
Table 4. Statistical variations in the cathedral frequencies in the summer and winter periods.
Monitored
period
Parameter
CV (%)
Summer
28/6-13/7/2011
Winter
27/1-9/2/2011
CV (%)
1
2,79
2
1,59
3
2,38
Mode no.
4
5
0,91
2,19
6
3,49
7
2,42
8
1,21
9,2
6,1
8,5
3,9
9,1
10,5
9,9
5,7
—
1,59
1,68
1,02
—
—
—
1,48
—
6,4
7,1
4,6
—
—
—
6,0
In Figures 14 and 15 the coefficients of correlation
between the natural frequencies of the cathedral and
the different temperatures are presented. For the
summer period and during the period of thermography monitoring, the eight modes were identified,
whereas, for the winter period only the modes number 2, 3, 4 and 8 were identified. The other modes
were local ones; therefore, their identification was
not always attainable as can be noticed in Figure 5. It
can be noticed for the summer and the winter periods that the coefficients of correlation with the stone
surface temperature were less than those with the
external and the internal temperature. In the summer period, the coefficients of correlation with the
external temperature were in average 0.57 and were
clearly higher than those with the stone surface temperature which were in average 0.25.
On the contrary, in the winter period the coefficients of correlation with the stone surface temperature were in average 0.56 and were not so far from
those with the external temperature which were 0.68
in average. The discussion given in the previous section (3.2) may explain this finding. The statistical
variations in the identified modes during the summer and winter monitored periods are reported in
Table 4.
For modes 2, 4 and 8 slightly higher changes
could be noticed in winter period than in summer
period. For mode 3 the contrary was found.
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Table 4. Statistical variations in the cathedral frequencies in the summer and winter periods.
Monitored
period
Parameter
CV (%)
Summer
28/6-13/7/2011
CV (%)
Winter
27/1-9/2/2011
1
2,79
2
1,59
3
2,38
Mode no.
4
5
0,91
2,19
6
3,49
7
2,42
8
1,21
9,2
6,1
8,5
3,9
9,1
10,5
9,9
5,7
—
1,59
1,68
1,02
—
—
—
1,48
—
6,4
7,1
4,6
—
—
—
6,0
4. CONCLUSIONS
An integrated inspection and monitoring program, encompassing different activities, has been
applied to Mallorca cathedral a large masonry historical structure built during the 14th – 16th c. The
AVT allowed for a good identification of the natural
frequencies of eight modes. The AVT was followed
by a continuous dynamic monitoring that worked
for about 15 months on a 24 h base. It confirmed the
results of the AVT by allowing the monitoring of the
evolution of the eight natural frequencies over time.
It was found that the changes in the natural frequencies of the cathedral, in terms of CV, were between
2.3 and 3.7%, and their percentual variation was between 10.4 and 18.5%.
A seasonal thermography monitoring (as a complementary study for the dynamic monitoring) was
used. An IR camera was installed in the winter and
the summer of 2011 for two weeks to monitor the
internal stone surface temperature of a large portion
of the cathedral. The correlation between the cathedral natural frequencies and the internal stone surface temperature of some selected structural elements was investigated. The correlation of the natu-
ral frequencies with the external and internal temperatures was also analyzed.
Concerning the correlation among the different
temperatures measure, the main conclusions are: I)
The internal stone surface temperature of the columns, vaults, arches and walls was in phase and
very near to each other; II) In summer, it was observed that the internal stone surface temperature
did not always vary according to the external temperature because the stone was not able to radiate
the stored heat as fast as the rapidly increasing external temperature; III) in winter, the stone surface
temperature was in phase with the external temperature.
Regarding the correlation between the natural
frequencies and the different measured temperatures, the thermography monitoring revealed an acceptable correlation between the stone internal surface temperature and the cathedral frequencies. In
the winter period higher correlation coefficients than
in the summer period were found. It was observed
also that the natural frequencies were more correlated with the external temperature then the internal
temperature and finally with the internal stone surface temperature.
ACKNOWLEDGMENT
This research has been carried out within the project “New Integrated Knowledge based approaches to
the protection of cultural heritage from Earthquake-induced Risk-NIKER” funded by the European Commission (Grant Agreement n° 244123), whose assistance is gratefully acknowledged. The authors also wish
to express their gratitude to the Chapter of Mallorca cathedral for the possibility of carrying out the present
study and the assistance received.
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