# Effects of Strongbacks and Strappings on Vibrations of Timber Truss Joist Floors

Authors: Shuo Xue; Zhanyi Zhang; Zhanyi Zhang; Haibin Zhou; Yinlan Shen
Journal: Shock and Vibration
 (2021)

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## Abstract

It is well known that the vertical vibrations of lightweight timber floors would cause discomfort to the occupants. As a new kind of flooring system, the metal-plate-connected timber truss joist floors were developed due to their larger spans and easier crossing of pipes and cables after sawn timber and I-joist floors. In this paper, the vibration modes and transfer functions of sixteen metal-plate-connected timber truss joist floors over a nominal span of 6 m were determined experimentally to measure the changes in vibration frequencies and transmissions obtained after the installation of strongbacks and strappings. The results showed that the fundamental natural frequencies of the metal-plate-connected timber truss joist floors at a 400 mm joist spacing were about 15 Hz, while the frequencies of the floors at a 600 mm joist spacing were about 12.5 Hz. The bracing elements of the strongbacks and strappings mainly enhanced the system stiffness in the across-joist direction of the flooring system, but they did not govern the fundamental natural frequencies of the floors and just changed the spacing of adjacent natural frequencies. The bracing elements as secondary elements of the floors also altered the vibration transmission paths in the across-joist direction. The frequencies where the stronger vibration transfers happened in the direction perpendicular to floor joists were generally above 15 Hz. Proper installation measurements of bracing elements in practical control need to be taken to alleviate the vibration response intensity at the targeted locations and frequencies.


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## Body

## 1. Introduction

Timber floors are by far the most common structural systems used in timber-framed buildings around the world [1]. Timber flooring systems are typically constructed with timber floor joists and wood-based sheathing. Compared with concrete floors, timber floors with lightweight construction have a low mass-to-stiffness ratio [2]. Problems regarding floor vibrations of timber floors are easily produced by the daily activities of occupants, such as walking, running, and jumping [3]. Because in a building the flooring system is only a structural system where occupants are in constant physical contact, the vertical vibration problem is a source of annoyance to occupants [4, 5]. Even though floor vibrations do not cause failure of a structure, it generally makes many people feel uneasy and will create fear of structural collapse, although such fear is unnecessary because of the small motions that are actually presented. Numerous efforts have been made to identify factors affecting human response to vibrations of joist-type floors [5–10]. It was concluded that frequency components, vibration amplitude, and damping of vibration were the most important factors affecting human response to vibrations [1]. The fundamental research for understanding the factors affecting human response to floor vibrations has paved the way for the development of design approaches to prevent annoying vibrations. With field investigations on the construction details and subjective evaluations on laboratory-constructed floors and floors in the occupied buildings, the correlations between human perceptions and vibration performances were statistically analyzed and some design criteria limiting the static deflection, vibration responses, or combination of some parameters were proposed [3, 5, 11–14]. These design approaches commonly targeted timber floors for different purposes to prevent objectionable vibrations.Whether these design criteria are rational to vibration serviceability of timber floors or not, it is primarily important for any timber floor design engineer to systematically clarify the performances of timber flooring structures on the vibration responses and build the corresponding relationships. The fundamental natural frequency of a timber floor is governed predominantly by the system stiffness in the joist direction [3, 6, 14, 15]. The spacing of two adjacent natural frequencies is controlled by the ratio of the perpendicular floor stiffness to the longitudinal floor stiffness [1]. Many construction details, such as floor decking thickness and material, attachment of floor decking to joists, lateral elements, and ceiling, contribute to the perpendicular floor stiffness. Natural frequencies, damping ratios, and mode shapes of a prefabricated floor element were influenced by floor fixing boundary conditions and construction stages [16]. The construction details, such as the way that components are attached and the boundary conditions at supports, can contribute to the Coulomb damping. The addition of dead loads, for example, installation of nonstructural elements, can also have considerable effects on the effective damping [7, 9, 16]. The presence of partitions on floors was found to provide exceedingly high damping [17].With the availability of engineered timber joists and trusses which evolved from traditional lumber joists, timber floor systems become longer span and continuous multispan systems. For architectural designers and structural engineers, the advent of stronger materials, lighter and more rigid cladding, smaller damping, longer spans, and more accurate strength calculations taking into account the interaction of components means that excessive vibrations now have a greater influence on structural design than before. Three types of parallel chord trusses, including glue-jointed timber trusses, open metal web trusses, and metal-plate-connected timber trusses, are generally used as timber floor joists in low-rise residential houses, benefited from large span, high strength, easy prefabrication, and convenience for crossing pipelines. Due to different structural compositions among joist products, the design methods based on other timber floors built from different joist products may have a discrepancy in vibration acceptability [18]. Timber truss joist floors are no exception. New construction practices have had a profound impact on the vibration characteristics of some timber floors [19]. Few literature works on the vibration performances of timber truss joist floors were reported. In terms of the glue-jointed timber truss joist floors, the second and third natural frequencies of the floors were significantly changed by installing strongbacks and strappings, indicating that the bracing elements increased the floor stiffness perpendicular to the joist direction [20]. With respect to open metal-web joists floors, the joist spacing and ceiling had no obvious influences on the fundamental natural frequency but had obvious influences on the natural frequencies of higher modes [21]. The dynamic responses of timber floors constructed with metal-web truss joists were also investigated by conducting field tests [9].Moreover, the perception of timber floor vibrations was usually subjectively evaluated from the walking person himself while ignoring the response of surrounding people. Vibration transfer in the flooring system should be considered especially for complex two-way timber truss joist floors with bracing elements in practical applications. It can determine the feasibility of some mitigation measures when the vibration responses are expected to be lessened at some locations in occupied truss joist floors with unacceptable vibrations or the design will be done to ensure the vibration responses at some interesting locations or paths under acceptable level for new timber truss joist floors. The acceleration responses from vibrations are not only related to the excitation intensity and the distance from the excitation point but also related to the floor structure. Although every excitation was from the same location, the acceleration at each response location is easily affected by the variation of the excitation intensity from these impacts [22]. The vibration transfer function of the floor is not affected by the excitation intensity, which can denote the transfer capacity to the vibration energy and transmission paths in the floor system [23]. Literature about the experimental impact assessments of structural changes on local and global vibration performances based on the vibration transfer function was limited for timber truss joist floors. In this paper, metal-plate-connected timber truss joist floors were constructed at the National Engineering Research Center of the Wood Industry in Beijing, China. The improvements in the vibration performances from the construction details including the spacings of joists and strappings and the location and number of strongbacks were systematically assessed in order to find floor construction methods known to reduce the amplitudes of dynamic motions and the derived characteristics like acceleration and avoid the construction details that cause direct vibration transmissions.


## 2. Construction of the Test Floors

All the test floors were originally transformed from two base test floors with different joist spacings. The transformations were achieved from the installation of bracing elements like strongbacks or strappings. These two base test floors were designed according to the ratio of the maximum floor deflection to the floor span to 1/360 under a uniform load of 1.9 kPa. The design span of the base test floors was 6 m. The joist spacing and width of one base test floor (T1) were 400 mm and 5.6 m, respectively, while the joist spacing and width of the other floor (T3) were 600 mm and 8.4 m. The base floor joists were the metal-plate-connected timber trusses with parallel chords. Each test floor was constructed from fifteen trusses which were evenly distributed. The metal plates for connecting the timber trusses were manufactured at a timber construction company according to the standard JGJ/T 265-2012 [24], and the truss sketch is shown in Figure 1. The length of the trusses for all test floors was 6 m and the height of the trusses was 438 mm. The flanges and webs of the truss were composed of 38 mm × 89 mm spruce-pine-fir (SPF) lumbers with J visual grade. According to the truss design, the precut flanges and webs at each node were connected with the galvanized metal connecting plates with a nominal thickness of 1 mm, a teeth length of 10.45 mm, a teeth width of 3.45 mm, and a teeth density of 106–108 No/dm2. The distance between adjacent nodes in the parallel direction was 500 mm. To check whether trusses met the design requirement, three timber trusses were randomly selected for the third-point loading test. The midspan deflections under a vertical point load of 2.51 kN, equivalent to a uniformly distributed load of 1.9 kPa on floors, were measures as 3.5 mm, 4.4 mm, and 3.9 mm, respectively.Figure 1
Typical parallel flange timber truss.The construction process of the base test floors is shown in Figure2. To easily measure the floor deflections and install the bracing elements at the bottom of the test floors, these base test floors were constructed on the wall framing with a height of 1.85 m. One door opening in one of four walls was prefabricated as the access to the experimenters. Each base test floor was composed of 15 truss joists. Each end of every truss joist was connected to the top plate of the exterior wall with 90 mm long lag screws. The bottom flange of the truss trimmer joist was fixed on the top plate of the wall with 70 mm long lag screws at 600 mm c/c. The rim joist was the laminated veneer lumber (LVL) with the strength grade of 8E-33f. The thickness of LVL was 38 mm and the height was 438 mm. The LVL header joist was connected to the end straight web of each floor joist with one 70 mm long screw on top and one on the bottom. Moreover, the LVL rim board was fixed to the top plate of the supported wall with 70 mm long screws at 600 mm c/c. After the installation of truss joists, the OSB floor decking was sheathed on the floor joists with 30 mm long screws at 150 mm c/c around the perimeter and at 300 mm c/c in the field. The physical and mechanical properties of the OSB floor sheathing met the requirements in the standard LY/T 2389-2014, as shown in Table 1. The thicknesses of the OSB boards were 15 mm for the joist spacing of 400 mm and 18 mm for the joist spacing of 600 mm. The layout of the OSB decking was perpendicular to the joist direction.Figure 2
Construction process of the test floors.
(a)(b)(c)(d)Table 1
Physical and mechanical properties of the adopted oriented strand boards (OSBs).
Thickness (mm)MOR∥ (MPa)MOR⊥ (MPa)MOE∥ (MPa)MOE⊥ (MPa)Density (kg/m3)1535.120.5428020806501835.322.652402400Note. MOE and MOR are the modulus of elasticity and the modulus of rupture, respectively; ∥ and ⊥ denote parallel (major strength direction) and perpendicular (minor strength direction) to the length direction, respectively.The base test floor with the joist spacing of 400 mm was called Floor T1, while another one with the joist spacing of 600 mm was named Floor T3. Before the installation of any bracing elements, two base test floors were named T1-1 and T3-1, respectively. Other test floors were evolved from these two base test floors T1-1 and T3-1, as listed in Table2. Floors T1-2 and T3-2 were installed on a strongback at the midspan of Floors T1-1 and T3-1. Floors T1-3 and T3-3 had two strongbacks at the midspan of Floors T1-1 and T3-1. Floors T1-4 and T3-4 had one strongback at the midspan and one at each quarter span of Floors T1-1 and T3-1. Finally, Floors T1-5 and T3-5 had two strongbacks at the midspan and one at each quarter span of Floors T1-1 and T3-1. The changes were the installations of the bracing elements of strongbacks and strappings, which can be seen in Figure 3. The strongbacks were the SPF lumbers with visual grade J and the section dimensions of 38 mm × 235 mm. These strongbacks were laid perpendicularly to the joist direction and fixed with screws to the straight web members of fifteen timber truss joists. The strappings were also the SPF lumbers with visual grade J and the section sizes of 19 mm × 89 mm. They were flatwise nailed to the bottom chords of these truss joists in the perpendicular direction to the joist direction. The spacings of the strappings were 300 mm, 400 mm, and 600 mm, respectively, for the two base test floors with different joist spacings.Table 2
Configuration details of the base test floors.
Floor typeJoist spacing (mm)Number of strongback rowsStrapping spacing (mm)T1-14000—T1-24001—T1-34002—T1-44003—T1-54004—T1-64000600T1-74000400T1-84000300T3-16000—T3-26001—T3-36002—T3-46003—T3-56004—T3-66000600T3-76000400T3-86000300Figure 3
Installation of the bracing elements of strongbacks and strappings onto the test floors. (a) Strongbacks. (b) Strappings.
(a)(b)


## 3. Test Methods

### 3.1. Modal Testing

The measurement grid on the test floors consisting of seven equally spaced rows along span direction and joist lines is shown in Figure4, and a total of 105 excitation locations were obtained. The five vibration response measurement locations were selected for attaining vibration response signals according to the asymmetric distribution and also by avoiding vibration nodal points, as seen in Figure 4. Five acceleration transducers (accelerometers) for vibration response measurement locations were mounted on the surface of the test floors. An exciting hammer with a rubber head was used to excite 105 excitation locations successively. Response data for each excitation was obtained by averaging the results from three repeated impact excitations. The test excitation and response signals were collected by using the INV3020C data acquisition system with 20 channels and the frequency response function was obtained. The measurements were checked and validated using the coherence function. The vibration mode shapes and their natural frequencies of the first three vibration modes of the test floors were analyzed by using the DASP-V10 analysis software available at the China Orient Institute of Noise and Vibration.Figure 4
The measurement grid of the test floors and response measurement locations.


### 3.2. Testing of the Transfer Function

Vibration transfer function tests on the floors were conducted to study the propagation attenuation characteristics of the vibration input signal for different floor configurations by adding transverse elements. The transfer function of the vibration mainly reflects the transmission characteristics of the vibration response in the system to the vibration excitation, which depends on the characteristics of the system itself and is not related to the input signal. If the input and output of the system arex (t) and y (t), the vibration transfer function is defined as the ratio of the Fourier transform Y (ω) of the output signal to the Fourier transform X (ω) of the input signal, with the mathematical expression as shown in(1)Hxyω=YωXω.Six acceleration transducers were arranged at the midspan of six-floor joists, shown in Figure5, where V is the excitation location, while P1, P2, P3, P4, P5, and P6 are the response measurement locations. P1 is adjacent to V, where the P1 response represents the input signal of the V excitation. When impacted at point V with the exciting hammer, the input signal at point P1 on the test floors and the output signals at points P2–P6 were measured.Figure 5
Locations of the hammer impact excitation and response measurements.


## 3.1. Modal Testing

The measurement grid on the test floors consisting of seven equally spaced rows along span direction and joist lines is shown in Figure4, and a total of 105 excitation locations were obtained. The five vibration response measurement locations were selected for attaining vibration response signals according to the asymmetric distribution and also by avoiding vibration nodal points, as seen in Figure 4. Five acceleration transducers (accelerometers) for vibration response measurement locations were mounted on the surface of the test floors. An exciting hammer with a rubber head was used to excite 105 excitation locations successively. Response data for each excitation was obtained by averaging the results from three repeated impact excitations. The test excitation and response signals were collected by using the INV3020C data acquisition system with 20 channels and the frequency response function was obtained. The measurements were checked and validated using the coherence function. The vibration mode shapes and their natural frequencies of the first three vibration modes of the test floors were analyzed by using the DASP-V10 analysis software available at the China Orient Institute of Noise and Vibration.Figure 4
The measurement grid of the test floors and response measurement locations.


## 3.2. Testing of the Transfer Function

Vibration transfer function tests on the floors were conducted to study the propagation attenuation characteristics of the vibration input signal for different floor configurations by adding transverse elements. The transfer function of the vibration mainly reflects the transmission characteristics of the vibration response in the system to the vibration excitation, which depends on the characteristics of the system itself and is not related to the input signal. If the input and output of the system arex (t) and y (t), the vibration transfer function is defined as the ratio of the Fourier transform Y (ω) of the output signal to the Fourier transform X (ω) of the input signal, with the mathematical expression as shown in(1)Hxyω=YωXω.Six acceleration transducers were arranged at the midspan of six-floor joists, shown in Figure5, where V is the excitation location, while P1, P2, P3, P4, P5, and P6 are the response measurement locations. P1 is adjacent to V, where the P1 response represents the input signal of the V excitation. When impacted at point V with the exciting hammer, the input signal at point P1 on the test floors and the output signals at points P2–P6 were measured.Figure 5
Locations of the hammer impact excitation and response measurements.


## 4. Results and Discussion

### 4.1. Effects of the Strongbacks and Strappings on the Vibration Modes of the Test Floors

The first three vibration mode shapes of the test floors are presented in Figure6. Although the test floors had different strongbacks/strappings or different joist spacings, all of them showed vertical vibrations and the first three vibration mode shapes among them were the same. The first vibration mode showed that the entire test floors sustained one vibration wave along the floor width direction. The second vibration mode exhibited two alternate vertical vibration waves of two adjacent floor parts along the floor width direction (perpendicular to the joist direction). Different from the first two vibration modes, the third vibration mode shape showed a three-part fluctuation along the floor width direction (the middle part and both edge parts with alternate vibrations).Figure 6
First three vibration mode shapes of the test floors. (a) Mode 1. (b) Mode 2. (c) Mode 3.
(a)(b)(c)The first three natural frequency components of the test floors with different installed strongbacks are shown in Figure7. For the test floors with the joist spacing of 400 mm, the fundamental natural frequencies of Floors T1-1 to T1-5 varied from 14.8 Hz to 15 Hz with the increase of the strongbacks. The second natural frequencies increased from 17.8 Hz to 20.6 Hz, while the third natural frequencies increased from 21.0 Hz to 27.4 Hz. One strongback at the midspan (Floor T1-2) only increased the second mode frequency by 1 Hz and the third mode frequency by 2.4 Hz, but almost no differences in the fundamental natural frequencies were observed, compared to the test floor without strongbacks (Floor T1-1). Two and three strongbacks at the midspan (Floor T1-3 and Floor T1-4) increased the second mode frequency by 1 Hz and 2.3 Hz, respectively; meanwhile, they increased the third mode frequency by 4.3 Hz and 4.4 Hz. Four strongbacks (Floor T1-5) increased the second mode frequency by 2.8 Hz and the third mode frequency by 6.4 Hz, while no differences in the fundamental natural frequency happened, compared to Floor T1-1.Figure 7
First three natural frequencies of the test floors with the joist spacings of 400 mm and 600 mm before and after the installation of strongbacks.
(a)(b)For the test floors with the joist spacing of 600 mm, the fundamental vibration frequencies of Floors T3-1 to T3-5 slightly increased from 12.2 Hz to 12.9 Hz with the increase of the number of strongbacks. The second natural frequencies increased from 16.9 Hz to 17.7 Hz, while the third natural frequencies increased from 17.5 Hz to 21.7 Hz. One strongback at the midspan (Floor T3-2) decreased the frequencies by 0.4 Hz and 0.2 Hz for the first and second modes, but increased the frequency by 2.5 Hz for the third mode, compared to the reference test floor without strongbacks (Floor T3-1). Four strongbacks (Floor T3-5) increased the frequency by 0.6 Hz for the second mode and by 4.2 Hz for the third mode, while the bracing elements decreased the fundamental frequency by only 0.1 Hz, compared to Floor T3-1.It can be seen that the fundamental vibration frequency for the first mode sustained no changes with the increase of strongbacks for the T1 and T3 test floor series. It was further proved that the fundamental vibration frequency was dominated primarily by the stiffness parallel to the joist direction [3, 6, 14, 15]. The bracing elements of strongbacks obviously raised the second and third natural frequencies [21]. The floors with the joist spacing of 400 mm sustained a greater change in the natural frequencies, compared with those with the joist spacing of 600 mm. This greatly widened the spacing of two adjacent natural frequencies, which was considered to induce human discomfort because of the development of beat frequencies [14]. Moreover, with the increase of the joist spacing for the same floor span, the natural frequencies of the test floors sustained decreases accordingly. The stiffness of each truss along to joist direction was about the same, but the system stiffness was reduced due to the decrease of the ratio of the span to the width. As shown in Figure 8, the static deflections at the center of the T1 test floor series were obviously smaller than these of the T3 test floor series.Figure 8
Midspan static deflections of the test floors before and after installation of strongbacks under the concentrated load of 1 kN at the floor center.
(a)(b)The changes of the first three natural frequency distributions for the test floors with and without strappings are shown in Figure9. For the test floors with the joist spacing 400 mm, the fundamental natural frequencies of Floors T1-6 to T1-8 decreased from 15.0 Hz to 14.7 Hz with the decrease of the strapping spacing. The second natural frequencies increased from 18.8 Hz to 19.2 Hz, while the third natural frequencies varied from 21.5 Hz to 25 Hz. For the test floors with the joist spacing of 600 mm, the fundamental natural frequencies of Floors T3-6 to T3-8 increased from 12.6 Hz to 12.9 Hz with the decrease of the strapping spacing, while the second and third natural frequencies varied from 16.3 Hz to 17 Hz and from 17.5 Hz to 18.0 Hz, respectively. Small changes in their frequencies from T3-6 to T3-8 floors were due to small differences in their stiffnesses as shown in Figure 10. Accordingly, the natural frequencies of the test floors with the 400 mm joist spacing were greater than those of the test floors with the 600 mm joist spacing. The decrease in the system stiffness contributed to the case. For the test floors with 400 mm and 600 mm joist spacings, their fundamental natural frequencies for the first vibration mode almost were unchanged before and after the installation of strappings. The second natural frequencies for the test floors with the 400 mm joist spacing increased by a few Hz after strappings were installed, while the second natural frequencies slightly decreased for the test floors with the 600 mm joist spacing. However, the second natural frequencies for the test floors with the 400 mm joist spacing had no significant changes for the strapping spacings of 600 mm, 400 mm, and 300 mm. The increase of rows of strappings just had an obvious influence on the third natural frequencies for the test floors with the joist spacing of 400 mm and caused a smaller effect on both the second and third natural frequencies for the test floors with the joist spacing of 600 mm.Figure 9
The first three natural frequencies of the test floors with the joist spacings of 400 mm and 600 mm before and after the installation of strappings.
(a)(b)Figure 10
Midspan static deflections of the test floors with the joist spacings of 400 mm and 600 mm before and after installation of strappings under the concentrated load of 1 kN at the floor center.
(a)(b)Similar to other floors, the main structural changes of the metal-plate-connected timber truss joist floors including the spacing of the joists or the system stiffness can affect the natural frequencies, static deflections, and dynamic responses. Moreover, the secondary structural changes including the amount and the location of strongbacks or strappings can also improve the vibration performances of the metal-plate-connected timber truss joist floors.


### 4.2. Effects of Strongbacks and Strappings on the Floor Vibration Transfer

When considering combined vibration endurance and transfer strength, the targeted frequency range from 5 Hz to 35 Hz was selected for the vibration transfer function tests. The coherence functions were determined at the resonance frequency according to the correlation between the excitation and response signals and all coherence coefficients were close to 1. This indicated that the vibration responses were better excited by the input excitation and the test results were validated. The transfer functions at each location along the midspan direction of the test floors with the 400 mm joist spacing before and after the installation of strongbacks were calculated and synthesized, as shown in Figure11. In general, the responses were attenuated with the increasing distance from the excitation source due to the geometrical damping, caused by the spreading of the vibration energy over a larger area, and the material damping, caused by the dissipation of the energy in these timber members, although the system damping ratios were below 10%. For Floor T1-2, one strongback put at the midspan caused the strong vibration energy to happen at the frequency of about 20 Hz, not only near the excitation location but also in the area far from the excitation location. Moreover, this seemed to defuse the vibration energy between 30 and 35 Hz. The location where strong vibration energy happened on Floor T1-3 presented a similar case with the vibration mode shape. The strongback distribution on Floor T1-4 caused the vibration energy to have a 500 mm wide gap at a distance of about 2 m from the excitation point but it appeared in a bigger area farther away. Floor T1-5 had just an obvious transmission path at about 21 Hz, caused by its second vibration mode. It can be thought that the vibration transfer is closely related to floor construction details, which altered the vibration natural frequencies [25].Figure 11
Transfer functions of the T1 test floors with the 400 mm joist spacing.
(a)(b)(c)(d)(e)The transfer functions at each location along the midspan direction of the test floors with the 600 mm joist spacing before and after the installation of strongbacks were calculated and synthesized, as shown in Figure12. It can be seen that, at second or higher natural vibration frequencies, the test floors had a strong vibration energy transfer path. At the third natural frequencies, the test floors had the greatest vibration amplitude in one area for Floor T3-1, two areas for Floors T3-2 and T3-5, and three areas for Floors T3-3 and T3-4. With the installation of strongbacks, the floor construction changed perpendicular to the joist direction and the strongback members played a bridging role in the vibration transmission. The vibration energy is transferred over a distance of more than 7 m by the bridge of strongbacks. After adding one or two strongbacks, the floors can transmit the strongest vibration energy; see Floors T3-2 and T3-3.Figure 12
Transfer functions of the T3 test floors with the 600 mm joist spacing.
(a)(b)(c)(d)(e)The transfer functions at each location along the midspan direction of the test floors with the 400 mm and 600 mm joist spacings before and after the installation of strappings were calculated and synthesized, as shown in Figures13 and 14. For the test floors with the 400 mm joist spacing, it can be seen that all the test floors had a strong vibration energy transfer path at frequencies above 20 Hz, especially this becoming more significant for the third natural frequency. The strappings were helpful to transmit the vibration energy at low frequencies below 20 Hz. The strong vibration energy transfer paths, which behaved in the third vibration mode shape, appeared at about 22 Hz with the decrease of the strapping spacing. The vibration transfer energy at about 25 Hz frequency for the floors with the strapping spacing of 600 mm was attenuated when the floors changed with the strapping spacings of 300 mm and 400 mm. For the test floors with the 600 mm joist spacing, the vibration transfer bands at the frequency range from 15 Hz to 30 Hz were widened and increased. However, the maximum vibration amplitude, when existing in the strongest vibration energy at some frequency, was effectively weakened to some extent.Figure 13
Transfer functions of the T1 test floors with the 400 mm joist spacing.
(a)(b)(c)(d)Figure 14
Transfer functions of the T3 test floors with the 600 mm joist spacing.
(a)(b)(c)(d)The amplitude distribution of the floor vibration transfer function was closely related to the vibration frequency and vibration mode of the test floors. The more the number of bracing elements, the more the scattered distribution of the peak amplitude for the vibration transmission in the interested frequency band. The frequency scope in which the stronger vibration transfer happened is above 15 Hz. The limit frequency of 15 Hz was lower than the second and third natural vibration frequencies. The vibration energy supporting the vibration amplitude can transfer a longer distance and cover the full width of the test floors. The bracing elements can also change the location where the peak vibration amplitude appears. The application of mitigation measurements can relieve the strong vibration response which may happen at some location or some frequency [26, 27].


## 4.1. Effects of the Strongbacks and Strappings on the Vibration Modes of the Test Floors

The first three vibration mode shapes of the test floors are presented in Figure6. Although the test floors had different strongbacks/strappings or different joist spacings, all of them showed vertical vibrations and the first three vibration mode shapes among them were the same. The first vibration mode showed that the entire test floors sustained one vibration wave along the floor width direction. The second vibration mode exhibited two alternate vertical vibration waves of two adjacent floor parts along the floor width direction (perpendicular to the joist direction). Different from the first two vibration modes, the third vibration mode shape showed a three-part fluctuation along the floor width direction (the middle part and both edge parts with alternate vibrations).Figure 6
First three vibration mode shapes of the test floors. (a) Mode 1. (b) Mode 2. (c) Mode 3.
(a)(b)(c)The first three natural frequency components of the test floors with different installed strongbacks are shown in Figure7. For the test floors with the joist spacing of 400 mm, the fundamental natural frequencies of Floors T1-1 to T1-5 varied from 14.8 Hz to 15 Hz with the increase of the strongbacks. The second natural frequencies increased from 17.8 Hz to 20.6 Hz, while the third natural frequencies increased from 21.0 Hz to 27.4 Hz. One strongback at the midspan (Floor T1-2) only increased the second mode frequency by 1 Hz and the third mode frequency by 2.4 Hz, but almost no differences in the fundamental natural frequencies were observed, compared to the test floor without strongbacks (Floor T1-1). Two and three strongbacks at the midspan (Floor T1-3 and Floor T1-4) increased the second mode frequency by 1 Hz and 2.3 Hz, respectively; meanwhile, they increased the third mode frequency by 4.3 Hz and 4.4 Hz. Four strongbacks (Floor T1-5) increased the second mode frequency by 2.8 Hz and the third mode frequency by 6.4 Hz, while no differences in the fundamental natural frequency happened, compared to Floor T1-1.Figure 7
First three natural frequencies of the test floors with the joist spacings of 400 mm and 600 mm before and after the installation of strongbacks.
(a)(b)For the test floors with the joist spacing of 600 mm, the fundamental vibration frequencies of Floors T3-1 to T3-5 slightly increased from 12.2 Hz to 12.9 Hz with the increase of the number of strongbacks. The second natural frequencies increased from 16.9 Hz to 17.7 Hz, while the third natural frequencies increased from 17.5 Hz to 21.7 Hz. One strongback at the midspan (Floor T3-2) decreased the frequencies by 0.4 Hz and 0.2 Hz for the first and second modes, but increased the frequency by 2.5 Hz for the third mode, compared to the reference test floor without strongbacks (Floor T3-1). Four strongbacks (Floor T3-5) increased the frequency by 0.6 Hz for the second mode and by 4.2 Hz for the third mode, while the bracing elements decreased the fundamental frequency by only 0.1 Hz, compared to Floor T3-1.It can be seen that the fundamental vibration frequency for the first mode sustained no changes with the increase of strongbacks for the T1 and T3 test floor series. It was further proved that the fundamental vibration frequency was dominated primarily by the stiffness parallel to the joist direction [3, 6, 14, 15]. The bracing elements of strongbacks obviously raised the second and third natural frequencies [21]. The floors with the joist spacing of 400 mm sustained a greater change in the natural frequencies, compared with those with the joist spacing of 600 mm. This greatly widened the spacing of two adjacent natural frequencies, which was considered to induce human discomfort because of the development of beat frequencies [14]. Moreover, with the increase of the joist spacing for the same floor span, the natural frequencies of the test floors sustained decreases accordingly. The stiffness of each truss along to joist direction was about the same, but the system stiffness was reduced due to the decrease of the ratio of the span to the width. As shown in Figure 8, the static deflections at the center of the T1 test floor series were obviously smaller than these of the T3 test floor series.Figure 8
Midspan static deflections of the test floors before and after installation of strongbacks under the concentrated load of 1 kN at the floor center.
(a)(b)The changes of the first three natural frequency distributions for the test floors with and without strappings are shown in Figure9. For the test floors with the joist spacing 400 mm, the fundamental natural frequencies of Floors T1-6 to T1-8 decreased from 15.0 Hz to 14.7 Hz with the decrease of the strapping spacing. The second natural frequencies increased from 18.8 Hz to 19.2 Hz, while the third natural frequencies varied from 21.5 Hz to 25 Hz. For the test floors with the joist spacing of 600 mm, the fundamental natural frequencies of Floors T3-6 to T3-8 increased from 12.6 Hz to 12.9 Hz with the decrease of the strapping spacing, while the second and third natural frequencies varied from 16.3 Hz to 17 Hz and from 17.5 Hz to 18.0 Hz, respectively. Small changes in their frequencies from T3-6 to T3-8 floors were due to small differences in their stiffnesses as shown in Figure 10. Accordingly, the natural frequencies of the test floors with the 400 mm joist spacing were greater than those of the test floors with the 600 mm joist spacing. The decrease in the system stiffness contributed to the case. For the test floors with 400 mm and 600 mm joist spacings, their fundamental natural frequencies for the first vibration mode almost were unchanged before and after the installation of strappings. The second natural frequencies for the test floors with the 400 mm joist spacing increased by a few Hz after strappings were installed, while the second natural frequencies slightly decreased for the test floors with the 600 mm joist spacing. However, the second natural frequencies for the test floors with the 400 mm joist spacing had no significant changes for the strapping spacings of 600 mm, 400 mm, and 300 mm. The increase of rows of strappings just had an obvious influence on the third natural frequencies for the test floors with the joist spacing of 400 mm and caused a smaller effect on both the second and third natural frequencies for the test floors with the joist spacing of 600 mm.Figure 9
The first three natural frequencies of the test floors with the joist spacings of 400 mm and 600 mm before and after the installation of strappings.
(a)(b)Figure 10
Midspan static deflections of the test floors with the joist spacings of 400 mm and 600 mm before and after installation of strappings under the concentrated load of 1 kN at the floor center.
(a)(b)Similar to other floors, the main structural changes of the metal-plate-connected timber truss joist floors including the spacing of the joists or the system stiffness can affect the natural frequencies, static deflections, and dynamic responses. Moreover, the secondary structural changes including the amount and the location of strongbacks or strappings can also improve the vibration performances of the metal-plate-connected timber truss joist floors.


## 4.2. Effects of Strongbacks and Strappings on the Floor Vibration Transfer

When considering combined vibration endurance and transfer strength, the targeted frequency range from 5 Hz to 35 Hz was selected for the vibration transfer function tests. The coherence functions were determined at the resonance frequency according to the correlation between the excitation and response signals and all coherence coefficients were close to 1. This indicated that the vibration responses were better excited by the input excitation and the test results were validated. The transfer functions at each location along the midspan direction of the test floors with the 400 mm joist spacing before and after the installation of strongbacks were calculated and synthesized, as shown in Figure11. In general, the responses were attenuated with the increasing distance from the excitation source due to the geometrical damping, caused by the spreading of the vibration energy over a larger area, and the material damping, caused by the dissipation of the energy in these timber members, although the system damping ratios were below 10%. For Floor T1-2, one strongback put at the midspan caused the strong vibration energy to happen at the frequency of about 20 Hz, not only near the excitation location but also in the area far from the excitation location. Moreover, this seemed to defuse the vibration energy between 30 and 35 Hz. The location where strong vibration energy happened on Floor T1-3 presented a similar case with the vibration mode shape. The strongback distribution on Floor T1-4 caused the vibration energy to have a 500 mm wide gap at a distance of about 2 m from the excitation point but it appeared in a bigger area farther away. Floor T1-5 had just an obvious transmission path at about 21 Hz, caused by its second vibration mode. It can be thought that the vibration transfer is closely related to floor construction details, which altered the vibration natural frequencies [25].Figure 11
Transfer functions of the T1 test floors with the 400 mm joist spacing.
(a)(b)(c)(d)(e)The transfer functions at each location along the midspan direction of the test floors with the 600 mm joist spacing before and after the installation of strongbacks were calculated and synthesized, as shown in Figure12. It can be seen that, at second or higher natural vibration frequencies, the test floors had a strong vibration energy transfer path. At the third natural frequencies, the test floors had the greatest vibration amplitude in one area for Floor T3-1, two areas for Floors T3-2 and T3-5, and three areas for Floors T3-3 and T3-4. With the installation of strongbacks, the floor construction changed perpendicular to the joist direction and the strongback members played a bridging role in the vibration transmission. The vibration energy is transferred over a distance of more than 7 m by the bridge of strongbacks. After adding one or two strongbacks, the floors can transmit the strongest vibration energy; see Floors T3-2 and T3-3.Figure 12
Transfer functions of the T3 test floors with the 600 mm joist spacing.
(a)(b)(c)(d)(e)The transfer functions at each location along the midspan direction of the test floors with the 400 mm and 600 mm joist spacings before and after the installation of strappings were calculated and synthesized, as shown in Figures13 and 14. For the test floors with the 400 mm joist spacing, it can be seen that all the test floors had a strong vibration energy transfer path at frequencies above 20 Hz, especially this becoming more significant for the third natural frequency. The strappings were helpful to transmit the vibration energy at low frequencies below 20 Hz. The strong vibration energy transfer paths, which behaved in the third vibration mode shape, appeared at about 22 Hz with the decrease of the strapping spacing. The vibration transfer energy at about 25 Hz frequency for the floors with the strapping spacing of 600 mm was attenuated when the floors changed with the strapping spacings of 300 mm and 400 mm. For the test floors with the 600 mm joist spacing, the vibration transfer bands at the frequency range from 15 Hz to 30 Hz were widened and increased. However, the maximum vibration amplitude, when existing in the strongest vibration energy at some frequency, was effectively weakened to some extent.Figure 13
Transfer functions of the T1 test floors with the 400 mm joist spacing.
(a)(b)(c)(d)Figure 14
Transfer functions of the T3 test floors with the 600 mm joist spacing.
(a)(b)(c)(d)The amplitude distribution of the floor vibration transfer function was closely related to the vibration frequency and vibration mode of the test floors. The more the number of bracing elements, the more the scattered distribution of the peak amplitude for the vibration transmission in the interested frequency band. The frequency scope in which the stronger vibration transfer happened is above 15 Hz. The limit frequency of 15 Hz was lower than the second and third natural vibration frequencies. The vibration energy supporting the vibration amplitude can transfer a longer distance and cover the full width of the test floors. The bracing elements can also change the location where the peak vibration amplitude appears. The application of mitigation measurements can relieve the strong vibration response which may happen at some location or some frequency [26, 27].


## 5. Conclusions

In this paper, the vibration modes and transfer functions of sixteen metal-plate-connected timber truss joist floors with the nominal span of 6 m were tested and the relationships among the bracing elements as secondary structural components, natural frequency changes, and vibration transmissions were analyzed. The main conclusions can be drawn as follows:(1)
The fundamental natural frequencies of the metal-plate-connected timber truss joist floors with the 400 mm joist spacing were about 15 Hz, while the frequencies of the floors with 600 mm joist spacing were about 12.5 Hz. The second natural frequencies of the metal-plate-connected timber truss joist floors with 400 mm and 600 mm joist spacings were above 17 Hz and 16 Hz, respectively. The third natural frequencies of the metal-plate-connected timber truss joist floors with 400 mm and 600 mm joist spacings were above 19 Hz and 17 Hz, respectively.(2)
The second and third natural frequencies of the floors could be significantly changed by adding the bracing elements of strongbacks and strappings. For the test floors with the 400 mm joist spacing, the second natural frequencies increased by 5.6% to 15.7% with the increase of the number of strongbacks, and the corresponding third natural frequencies increased by 11.4% to 30.5%. With the decrease of the strapping spacing, the second and third natural frequencies did not show evident changing trends.(3)
Main transmission paths of the vibration energy in the across-joist direction depended on natural vibrations of the floors caused by the input excitation. The frequency scope in which the stronger vibration transfer happened was generally above 15 Hz. The more the number of bracing elements, the more the scattered distribution of the peak amplitude for the vibration transmission in the interested frequency band. The bracing elements effectively changed the locations for the peak vibration amplitudes and their vibration intensities.(4)
The bracing elements as secondary structural components of the floors enhanced the stiffness in the across-joist direction and altered the vibration transmission paths. The stiffnesses of the floor systems influenced their vibration modes and vibration transmissions. Effective mitigation measurements should be selected to relieve the strong vibration responses at some locations for some frequency.



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*Source: 6630719-2021-07-07.xml*