Introduction

In the last decade, the occurrence of damages and cracking on architectural heritage buildings due to seismic events and/or overloading, has stimulated research on masonry structures to define procedures able to protect such structures.

The protection of the architectural heritage against seismic events has become a strategic point for the territorial planning. This is especially required for all those countries that possess a wide and rich historical patrimony and which, on the other hand, are characterized by a high seismic risk, such as Italy. In this field, two different aspects have been studied by the researchers: the technical solutions for the protection of such structures (Modena et al. 2002; Osmancikli et al. 2012; Valluzzi et al. 2005; Lourenco 2005), and the problems connected with the definition of a model able to predict the structural response (D’Ambrisi et al. 2012; Diaferio et al. 2014a, 2016; Foti et al. 2015; Russo et al. 2010).

Due to an un-normalized constructive process, in fact, the Italian heritage includes a wide range of different typologies of masonry buildings that have not been designed to resist to the horizontal actions as those due to earthquakes. Among these construction typologies, the ones characterized by a high flexibility are particularly vulnerable to the seismic events, as they may show large amplitude oscillations incompatible with the mechanical properties of their structural elements (Ahmadi et al. 2014; Bartoli et al. 2013; Diaferio et al. 2014b; Foti 2014, 2015; Gentile and Saisi 2007; Tomaszewska and Szymczak 2012). A widespread typology is the bell tower, in particular, here the bell tower of the Trani’s (Apulia, Italy) Cathedral is considered. As a consequence of the interventions done during the years, the tower is actually characterized by walls whose core is realized in concrete while the external facades are made with the original Trani stones.

Moreover, the examined structure, due to its slenderness, may be vulnerable to lateral loads, and consequently an accurate analysis is required.

The present paper deals with the definition and development of a numerical model of the bell tower and with its analysis for the evaluation of the seismic performances of this historical masonry tower. Unfortunately, all the necessary information were not available due to the lack of documents. In addition, the mechanical properties of the structural materials are unknown, because the structure is subjected to degradation phenomena and cracking. Another element of uncertainty is represented by the interaction with the surrounding Cathedral, and the presence of inhomogeneities, etc. The aforementioned problems commonly occur during the evaluation of the vulnerability of a historical building, therefore the examined case may be representative of a class of buildings.

In these cases, the approach may be oriented to the implementation of a wide experimental campaign that by means of ground penetrating radar tests, thermografy, etc. (Binda et al. 1998, 2005; Diaferio et al. 2015b), may give information regarding the local properties of the structure. Numerous procedures have been proposed for the evaluation of the mechanical properties of the structural materials and the mapping of the holes or the construction details that can be adopted also in the cases in which retrofitting interventions have been done (D’Ambrisi et al. 2012; Modena et al. 2002; Osmancikli et al. 2012). Nevertheless, as the dimensions of the examined structure increase, the possibility of evaluating all the required information for the definition of a numerical model—on which dynamic analysis could be performed—becomes cumbersome and other approaches have to be implemented.

In this field, the dynamic tests, the subsequent structural identification and the updating of a numerical model of the structure to match the experimental results (Diaferio et al. 2015c; Gentile and Saisi 2013; Ivorra and Pallares 2006; Ivorra et al. 2016; Ramos et al. 2010) is the most widely diffused approach. In fact, even if this approach gives information regarding the local properties of the structure less accurate than the ones supplied by the procedures in (Binda et al. 1998, 2005; Diaferio et al. 2015a, b, c), on the other hand, it is able to give a detailed description of the global behavior of the structure that can be used for judging its safety level and be a useful tool for decision makers.

The use of dynamic tests, modal identification and subsequent updating of a numerical model of the structure has been also proposed in the literature for the estimation of the constraint conditions due to the interaction between the examined tower and the surroundings structures (Diaferio et al. 2016; Gentile and Saisi 2007).

Due to the complexity of Trani’s bell tower, with walls made by coupled concrete and masonry materials and unknown connections with the contiguous Cathedral, the numerical model has been validated by means of a comparison with the results of a wide experimental campaign. In situ tests have been conducted both by “local” non-destructive methods, such as ground penetrating radar (GPR) tests, and “global” methods, such as dynamic tests performed in operational conditions.

The main purpose of the present paper is to investigate the seismic vulnerability of the tower by means of such reliable numerical model experimentally validated, in accordance with the Italian guidelines for seismic risk assessment and mitigation of cultural heritage.

Trani’s Cathedral bell tower

Trani’s Cathedral is one of the most significant structures in Apulian Romanesque style (Fig. 1); its construction began at the end of the eleventh century and ended in 1143. The bell tower was built starting in 1240 and ended in the second half of 1300.

Fig. 1
figure 1

Trani’s Cathedral and its bell tower

Trani’s Cathedral bell tower has a square transversal section, above the pointed arch that connects the tower to the Cathedral. Up to the arch, at a level of about 14.30 m, there is a rigid floor in correspondence of the opening that connects the bell tower to the church.

From this level upwards, the square plan section with 7.50 m side remains constant for five floors up to the quote of about 47.6 m. At the top, the tower section becomes octagonal with a side of about 2.3 m.

The octagonal section remains constant up to the quote of about 51 m up to which the dome emerges.

The total height of the tower is 57 m, the walls thickness in correspondence of the square plan section is about 1.40 m.

The first two floors show on each façade round arched mullioned windows, while at the third and fourth levels, respectively, three- and four-light windows are present, while the upper floor (fifth level) is characterized by five-light windows.

During the years, the tower has been subjected to numerous structural interventions; in fact, since from 1700 the tower has exhibited static problems. However, the most severe intervention has been performed in the 1950, when the tower was completely disassembled, and a concrete core was built for reducing its oscillations. The tufa masonry (Trani stone) blocks were reassembled on the concrete core in the same original position.

The finite element model

To define a refined three-dimensional finite element (FE) model of the examined bell tower, an accurate analysis of the available historical documents and drawings has been executed. Nevertheless, due to the lack of information regarding the mechanical properties of the structural materials, the dimensions of the concrete core, and the constraint conditions due to the connection with the Cathedral, an extensive experimental campaign has been performed. In detail, a preliminary geometric survey and ground penetrating radar (GPR) tests have been conducted at each level of the tower.

In detail, the system IDS HI-MOD with a high frequency transmitter and receiver antenna (2 GHz) has been used, and the investigation has been considered 1 m of depth of the walls. Several acquisitions have been carried out at different levels of the tower and moving the radar following a line on the wall. The results demonstrate the presence in the core of the walls of material less coherent than the external surface, the latter one, whose thickness is about 25 cm, is characterized by regular and squared blocks of good quality and good consistency.

Then, dynamic tests in operational conditions have been performed by means of a monitoring system, consisting into 28 PCB (Model 393B31) uniaxial piezoelectric accelerometers connected to four digital acquisition systems connected to a laptop by an ethernet cable. The accelerometers were placed on four different levels of the tower. Eleven consecutive tests were conducted on the tower; each test had duration of 10 min with a sampling frequency of 1024 Hz, which has been subsequently decimated by a factor equal to 4 to have a frequency of 256 Hz. The acquired data have been analyzed by means of two operational modal analysis techniques (Diaferio et al. 2015b): one that operates in the frequency domain and the other one in the time domain. Table 1 shows the identified natural frequencies that have been evaluated as mean values of the identification results obtained analyzing all the acquired data during the numerous dynamic tests performed on the bell tower.

Table 1 Results of the modal identification: estimated frequencies for each natural mode

Based on the available information a three-dimensional FE model has been defined by means of Straus Software package (Straus7). The tower has been modeled with 8-nodes 4093 plate elements (QUAD8) that can better describe the behavior of thick plates like the ones here considered (Fig. 2); such shell element is a quadrilateral element which assumes as nodes the four corners and other four extra nodes along the four edges. The tower has been considered fully fixed at the base, while its connection with the adjacent Cathedral has been modeled by means of springs. Moreover, the stairs and the bells have been neglected into the FE model as their values are not significant respect to the structural mass. The thickness of the shell elements has been defined in accordance with the available drawings.

Fig. 2
figure 2

FE model of Trani’s Cathedral bell tower

The walls have been modeled with a homogeneous material. In fact, as confirmed by GPR tests, there is a perfect connection between the external Trani’s stones and the concrete core. Consequently, the walls have been modeled with a uniform material whose mechanical properties (i.e., density and elastic modulus) have been obtained by weighted averaging of the contributions of the stones and the concrete with respect to the thickness of each material into the wall. In detail, taking into account the values connected to the different levels of the tower, the density values range between 2460 and 2600 kg/m3, while the elastic modulus between 3200 and 24,000 MPa the first one related to the masonry walls and the second one to the concrete core. In detail, at the levels with a square plan the adopted density is 2485 kg/m3 and the Young’s modulus is 18,270 MPa, while at the top of the tower where the transversal section changed, it has been adopted a density equal to 2600 kg/m3 and a Young’s modulus equal to 3200 MPa.

The spring stiffness that models the constraint due to the connection with the surrounding Cathedral has been also chosen to match the experimental results. Table 2 shows the experimental frequencies and the numerical ones.

Table 2 Comparison between experimental and numerical frequencies for each one of the first five modes

In Fig. 3, the first two natural mode shapes are sketched.

Fig. 3
figure 3

a The first mode shape f 1 = 2.04 Hz; b the second mode shape f 2 = 2.25 Hz

The considered static loads acting on the tower are due to self-weights and live loads (5 kN/m2).

The seismic hazard

Trani’s area is a seismic prone zone. According to the seismic Italian code (NTC 2008; DPCM 2011), the site is characterized by the hazard curve in Fig. 4, where the PGA at the bedrock a g is plotted varying the return period T R. The PGA at the bedrock with a 475 years return period is equal to a g = 0.145 g. For the site effect, a rock mass has been assumed for the subsoil condition and a flat land for the topographic condition; on such basis an amplification factor S = 1.0 has been adopted in accordance with the Italian building code (NTC 2008; DPCM 2011).

Fig. 4
figure 4

Seismic hazard curve at the bell tower site

The behavior factor has been assumed equal to 2.25 that is the value suggested by the Italian building code (NTC 08) for towers irregular in elevation like in the case here considered, which is characterized by the presence of the Cathedral only on one side of the tower. In Fig. 5. the elastic response spectrum S e and the design response spectrum related to the horizontal direction S d are shown for the life safe limit state.

Fig. 5
figure 5

Elastic and design response spectra for life safe limit state

Static and seismic analysis

A preliminary linear static analysis has been performed on the FE model of the tower, assuming the tower fully fixed at the base and by simulating the interaction with the adjacent Cathedral by means of springs, as aforementioned. The tower has been considered subjected to self-weights and live loads (the latter equal to 5 kN/m2), the evaluated normal stresses are shown in Fig. 6. It can be observed that the values are compatible with the ordinary resistances of concrete and masonry materials (≅25 N/mm2).

Fig. 6
figure 6

Normal stress pattern due to static loads

Moreover, the model has been subjected to the design spectra in Fig. 5. The walls have been verified; in Fig. 7b an example of the performed analysis is shown for the wall at the first floor, the latter reported in Fig. 7a.

Fig. 7
figure 7

a In the black rectangular the considered wall; b normal force–moment domain, in blue the stress condition

A nonlinear static analysis has been performed by adopting lateral forces distributed linearly along the height of the tower; in detail, the introduced forces are proportional to the masses and to the displacements of the normalized first mode of the structure in the considered direction:

$$F_{i} = \left( {S_{d} \left( {T_{1} } \right)\frac{W\lambda }{g}} \right)\frac{{W_{i} z_{i} }}{{\mathop \sum \nolimits_{j = 1}^{n} W_{j} z_{j} }} = F_{h} \frac{{W_{i} z_{i} }}{{\mathop \sum \nolimits_{j = 1}^{n} W_{j} z_{j} }},$$
(1)

where W is the total mass, W i and \(z_{i}\) are the mass and the height at the ith level, g is the gravity acceleration and \(S_{\text{d}} (T_{1} )\) is the design acceleration evaluated in accordance with the design response spectrum and referred to the first period of the tower, and λ is the coefficient that depends on the geometrical characteristics of the structure. For the case here considered F h is equal to 2019 kN.

Figure 8 shows the stress–strain relationship that has been adopted for describing the nonlinear behavior of the structural material.

Fig. 8
figure 8

Stress–strain relation of the structural material

The pushover analysis has been carried out up to the collapse, which has been characterized taking into account different criteria to compare the results.

As a first step, the Rankine criterion (maximum stress) has been adopted as yield criterion.

Analyzing the distribution of the stress along the tower during the sequence of load increment, it can be verified that at the 12th step the maximum compressive strain is reached in correspondence of a load that is 20% greater than the load of life safe limit state (Fig. 9).

Fig. 9
figure 9

Stress pattern of nonlinear static analysis (Rankine criterion)

Moreover, the maximum tensile stresses appear at the 8th step that is in correspondence of a load equal to 80% of the load for the life safe limit state (Fig. 10).

Fig. 10
figure 10

Stress pattern of nonlinear static analysis (maximum tensile stress)

The nonlinear static analysis has been performed also adopting, as yield criterion, the Coulomb criterion:

$$\tau = c + \sigma {\text{tg}}(\varphi ),$$
(2)

where \(\tau\) is the shear stress, and it has been assumed c = 0.37, σ = 0.64 MPa and \({\text{tg(}}\varphi )= 0.4.\) Thus, the limit value for the shear stress is equal to 0.29 MPa. Figure 11 shows the stress pattern of the tower the zones where the maximum shear stress compatible with the Coulomb criterion is achieved, can be observed.

Fig. 11
figure 11

Stress pattern of nonlinear static analysis (Coulomb criterion)

Above three risk assessment criteria have been analyzed: Rankine criterion, maximum tensile stress and Coulomb criterion. To verify the actual safety level of the bell tower in the following, the three above mentioned criteria have been compared and the safest one has been adopted as risk assessment criteria.

In Fig. 12, the capacity curve (number of the load step increment vs. the maximum displacement of the center of mass of the upper level) of the examined bell tower is shown, and the displacement capacity, evaluated for each one of the aforementioned criteria, is plotted.

Fig. 12
figure 12

Capacity curve of the bell tower

The maximum tensile stress criterion is the one that estimates the lower displacement capacity; consequently, it is the one adopted as risk assessment criteria.

The pushover curve has been managed to evaluate the curve of the equivalent Single Degree of Fredom (SDOF) system.

In accordance with the Italian building code (NTC 2008), the base shear force F and the roof displacement d obtained by the pushover analysis have to be converted into the corresponding modal force F* and displacement d* of the equivalent SDOF system, as follows:

$$d^{*} = \frac{d}{\varGamma }\quad F^{*} = \frac{F}{\varGamma },$$
(3)

where Γ is the modal participation factor.

On such basis the equivalent SDOF system has been defined in accordance with the Italian building code (NTC 2008; DPCM 2011). Figure 13 shows the comparison between the capacity curve of the tower and the bilinear curve of the equivalent SDOF system. The bilinear curve gives a behavior factor that is defined as the ratio between the maximum displacement and the yielding displacement equal to 1.34, lower than the value suggested by the Italian code (NTC 08).

Fig. 13
figure 13

Comparison between the capacity curve of the tower (blue line) and the bilinear curve of the equivalent SDOF system (green line)

The period of the SDOF system T* is

$$T^{*} = 2\pi \sqrt {\frac{{m^{*} }}{{k^{*} }}} ,$$
(4)

where \(m^{*} = \mathop \sum \nolimits m_{i } \phi_{i}\), m i is the mass at the ith floor level of the tower, ϕ i is the ith component of the first eigenvector, and k* is the elastic stiffness of the equivalent bilinear curve. In the present case study, it has been obtained T* = 0.4 s.

The seismic displacement demand evaluated in accordance with the Italian code is 0.4 m, higher than the maximum displacement estimated by means of the pushover analysis.

Conclusions

A nonlinear pushover analysis procedure has been applied to study the seismic vulnerability and quantify the failure risk of the Trani Cathedral’s bell tower, one of the most important heritage buildings in Apulian Romanesque style. The tower is constituted by walls composed by a concrete core and external layers made by Trani stone.

A three-dimensional finite element model of the tower has been defined on the basis of an extensive experimental campaign and validated by means of dynamic tests under ambient forces. Ground penetrating radar tests have been carried out too to get more information and to appropriately calibrate the 3D finite element model.

Three risk assessment criteria (Rankine criterion, maximum tensile criterion and Coulomb criterion) have been compared and the safest one has been adopted to evaluate the displacement capacity of the bell tower and its seismic vulnerability. Then the capacity curve of the examined structure has been evaluated considering the life safe limit state and analyzing the possible global collapse mechanisms.

The vulnerability analysis has shown that the seismic displacement demand, evaluated in accordance with the Italian Building Code for seismic hazard of Trani, is higher than the maximum displacement capacity obtained adopting the maximum tensile stress criterion.