Advertisement

3D network structure and sensing performance of woven fabric as promising flexible strain sensor

  • 214 Accesses

Abstract

A flexible strain sensor was developed through weaving conductive yarns to 3D woven fabric. The relationship between the sensing performance of the woven fabric and its 3D network structure containing yarn shrinkage and arrangement density, as well as fabric interweaving, was investigated according to Pierce’s fabric geometry model and the assumption of elastic strain of yarn. Based on such models and assumption, the theoretical results were verified by the experimental data from uniaxial stretching, and the trends of both results were consistent. The sensitivity of woven fabric on its elastic strain is relatively small (GF < 2) and nonlinearity. With the deformation of fabric geometry structure (Stage I) caused by stretching on warp direction, the shrinkage of weft yarn (cw) and interweaving points (nw) decreased or the arrangement density of warp yarn (Nj) increased, resulting in improved sensitivity on warp direction. At yarn deformation stage (Stage II), the increase in interweaving points (nw) or the decrease in arrangement density of warp yarn (Nj) could improve the sensitivity on warp direction. All the results provide a theory basis for the design and development of flexible strain sensor with promising application as wearable electronic device.

Introduction

Recently with the rapid development of wearable electronic devices, more researches were focused on textile-based electronic named electronic textiles (E-textiles) [1,2,3,4,5]. Because it was made of flexible materials and special 3D network structure, E-textiles not only fit the comfort requirement of human body, but also can adapt to strain caused by human body movement. Unfortunately, our daily textiles did not have electrical functions especially sensing performance. To achieve full E-textiles systems, it was necessary to integrate the advantages of 3D network of textiles with electronic functions. During the past decade, a large amount of approaches had been tried and now two different featured E-textiles systems had been developed. One was to embed the simple electronic devices onto off-the-shelf textiles substrates [6,7,8]; the other was to integrate the electronic function with fibers which can be further processed to textiles [9, 10]. Although the integration of simple electronic devices onto textile substrate was easier to fabricate, the accessibility, comfort, durability, flexibility and stretchability of prepared E-textiles are extremely deteriorated due to mismatch between rigid electronics devices and flexible textiles [11]. On the contrary using textile technology was more suitable for processing the flexible fiber with electronic function to complex structure and area-scalable E-textiles [12].

Fabric as one of the main textiles, if made from flexible and electrical yarns had been demonstrated sensing performance because of its 3D network structure. Sensitivity was normally introduced to evaluate the sensing performance which is expressed as gauge factor (\({\text{GF}} = \frac{dR}{R\varepsilon }\), where dR is the change rate of resistance, R is the initial resistance, and ε is applied strain) [13]. Three main 3D network structures of fabric (woven, knitting, and non-woven) can be used as strain sensor of E-textiles, of which woven fabric sensor was characterized by relatively high sensitivity and low stretchability due to the relatively tight texture [14,15,16,17]. Du et al. [15] prepared a non-woven structure-based strain sensor by coating graphene on the surface of non-woven fabric which exhibited a relatively low sensitivity (GF < 7.1) and low stretchability (ε < 10%). Seyedin et al. [18] used the electrical conductive PU/PEDOT: PSS fibers to fabricate knitting structure-based strain sensor which exhibited high stretchability (strain up to 160%) but relatively low sensitivity (GF = 1). Yan et al. [19] prepared woven structure-based strain sensor by carbonizing polyacrylonitrile nanofiber yarns of fabric which exhibited high sensitivity (GF = 77.3) and relatively low stretchability (strain < 12%). For above sensing performance, E-textiles based on woven structure can accurately monitor the small strain such as heartbeat, pulse, and voice facial expression recognition due to its relatively high sensitivity [20,21,22]. However, at present there were few studies on the influence of woven fabric geometric structure change and yarn deformation on its sensing performance. Ma et al. [23] studied the resistance of woven fabric and its change during stretching only on the experiment results, but the relationship between fabric structure parameters and resistance changes had not been studied. In order for the well application of woven fabric strain sensors based on its 3D network structure, it is necessary to study the relationship between the structure parameters of woven fabric and its sensing performance under stretching.

In this work, the Pierce fabric geometry model was introduced for the first time to study the relationship between sensing performance and network structure parameters of woven fabric [24]. At first the relationship between the interlacing rules of warp and weft yarns and the electrical conductivity of woven fabrics was studied. Then, the geometric structure model of Pierce was introduced to study the relationship between sensing performance and structure parameters on uniaxial stretching and the mathematical relationship was derived. Finally, the reliability of the above results was verified experimentally. We expected these studies can guide the design, development and application of woven fabric strain sensor based on its 3D network structure.

Materials and methods

Materials

The electrical conductive yarn (plied yarn) made of silver nanoparticles (AgNPs)-coated polyester staple yarns by ply twisting was kindly supplied by Shenzhen Huizheng new materials Ltd. China. (Fineness 120tex, Coefficient of twist 260 ± 10, Density 0.93 g/cm3, Diameter 0.40 mm).

Measurement for the electrical resistance of yarn

The axial and radial resistance of yarn was measured, respectively, by Keysight 34461A universal digital meter (Digital multi-meter, 34461A, Agilent Technologies Inc. USA.); each sample was tested three times to get the average value. The axial and radial resistivity \(\rho_{\text{a}} ,\rho_{\text{r}}\) can be derived by equation \(R = \rho \frac{L}{S}\) (Support Information S1).

Preparation of woven fabric

As shown in Fig. 1, the electrical conductive yarns were fabricated to 3D network structure of woven fabric by semi-automatic sample loom (Y208W Changzhou No.2 textile instrument factory China). The arrangement density of warp and weft is 100–110 roots/10 cm and 90–100 roots/10 cm, respectively; the woven fabric structure is \(\frac{ 1}{1}\) plain weave and \(\frac{1 }{ 2} \nearrow\) twill weave for comparison.

Fig. 1
figure1

3D network of woven fabric as aplain weave, b twill weave

Measurement of the electro-mechanical performance of woven fabric under uniaxial stretching

The strain (\(\varepsilon_{\text{j}}\)) of woven fabric was measured using Instron 5943 Tensile Testing Machine (Instron Inc. UK) according to ASTM D882-10 at room temperature, while the resistance change rate \((dR/R_{0} )\) was measured by Keysight 34461A universal digital meter (Digital multi-meter, 34461A, Agilent Technologies Inc. USA). The sensitivity index of gauge factor \(({\text{GF}} = dR/R_{0} \varepsilon )\) was used to evaluate the sensing performance of woven fabric strain sensor. The measurement of strain on weft direction \(\left( {\varepsilon_{\text{w}} } \right)\), the shrinkage of warp and weft yarn \((c_{\text{j}} ,c_{\text{w}} )\) during stretching on warp direction can be reviewed on Support Information S2.

Result and discussion

The electrical resistance of conductive yarns

Woven fabric is made by interweaving two sets of electrical conductive yarns that intersect vertically (warp and weft); electric currents can flow through the axial direction of the yarns or through from the radial direction of one set of yarns to another. As shown in Fig. 2a, the axial resistance of the yarns (Ra) can be expressed according to the mathematical expression of the surface specific resistance as

$$R_{\text{a}} = \rho_{\text{a}} \frac{L}{S} = 4\frac{{\rho_{{{\text{a}} }} L}}{{\pi D^{2} }}$$
(1)

where \(\rho_{\text{a}}\) is the axial resistivity of yarn; L is the length of yarn; S is the area of yarn cross section \(S = \frac{\pi }{4}D^{2}\); and D is the diameter of yarn.

Fig. 2
figure2

Graphic analysis of a axial resistance, b radial resistance, c the parallel of radial resistor, d contacted resistance of Rcw, e contacted resistance of Rcj

Accordingly the axial resistances of warp and weft yarns can be expressed as:

$$R_{\text{aj}} = \frac{{4\rho_{\text{a}} L_{\text{j}} }}{{\pi D_{\text{j}}^{2} }}; \quad R_{\text{aw}} = \frac{{4\rho_{\text{a}} L_{\text{w}} }}{{\pi D_{\text{w}}^{2} }}$$
(2)

where Dj and Dw are the diameters of warp and weft; Lj and Lw are the lengths of warp and weft.

As shown in Fig. 2b, the radial resistance of yarns can be viewed as a series of small radial resistors with angle dθ in parallel and the resistance of each resistor (Ri) can be expressed as

$$S = L \times r{\text{d}}\theta ;\quad R_{i} = \rho_{\text{r}} \frac{r}{{Lr{\text{d}}\theta }} = \rho_{\text{r}} \frac{1}{{L{\text{d}}\theta }}$$
(3)

where \(\rho_{\text{r}}\) is the radial resistivity of the yarn; r is the radius of yarn; and L is the length through which radial current flows.

Because the radial resistor with angle dθ is in parallel (Fig. 2c), the total radial resistance Rr of yarn can be expressed as:

$$\frac{1}{{R_{\text{r}} }} = \sum \frac{1}{Ri} = \frac{L}{{\rho_{\text{r}} }}\sum {\text{d}}\theta = \frac{L}{{\rho_{\text{r}} }}\int_{0}^{2\pi } {\text{d}} \theta = \frac{2\pi L}{{\rho_{\text{r}} }}; \, \quad R_{\text{r}} = \frac{{\rho_{\text{r}} }}{2\pi L}$$
(4)

On woven fabric, the electric currents flow through from one set of yarns to another; the resistance is related to the angle of contact at which the yarns intersect. The resistance where the current flows radially from weft to the warp is called the contact resistance Rcw (Fig. 2d), while the resistance where the current flows radially from warp to weft is called the contact resistance Rcj (Fig. 2e). According to Eq. (4), Rcj and Rcw can be expressed as:

$$R_{{\text{cw}}} = \frac{{\rho_{\text{r}} }}{{\theta_{{\text{w}}} D_{{\text{w}}} }}; \quad R_{{\text{cj}}} = \frac{{\rho_{\text{r}} }}{{\theta_{{\text{j}}} D_{{\text{j}}} }}$$
(5)

where θj is the contacted angle of warp covers on weft; θw is the contact angle of weft covers on warp; and the diameters of warp and weft Dj and Dw correspond to L of Eq. (4).

The resistance of woven fabrics on warp and weft direction

As shown in Fig. 3a, when the resistance on the warp direction measured on both ends of the warp can be regarded as two equal potential points, the resistance of the whole warp system can be approximately regarded as the resistance of the fabric on warp direction. Similarly, the resistance of the whole weft system can be approximately regarded as the resistance of the fabric on the weft direction. The resistance of warp system (Rj) contains the sum of the resistances of the two current paths; one is currents directly flowing through whole warp yarns (Rj→j), the other is the currents flowing from weft to warp (Rw→j), where weft was interwoven with warp. As shown in Fig. 3b, c, the Rj→j can be regarded as each warp resistor in parallel, while the Rw→j can be regarded as each weft resistor in parallel. The resistance of each weft is the sum of the contact resistance where the weft interwoven with the warp (Rcw) and the resistance of the weft (Raw).

$$R_{\text{j} \to \text{j}} = \frac{{R_{{{\text{aj}}}} }}{{N_{{\text{j}}} }}; \quad R_{\text{w} \to \text{j}} = \frac{{R_{{\text{cw}}} + R_{{{\text{aw}}}} }}{{n_{{\text{w}}} }};\quad R_{{\text{j}}} = R_{\text{j} \to \text{j}} + R_{\text{w} \to \text{j}} = \frac{{R_{{{\text{aj}}}} }}{{N_{{\text{j}}} }} + \frac{{R_{{\text{cw}}} + R_{{{\text{aw}}}} }}{{n_{{\text{w}}} }}$$
(6)

where Raj and Raw are the axial resistance of each warp yarn or weft yarn according to Eq. (2); Rcw is the contact resistance of each interlacing point, where current flows through weft to warp according to Eq. (4); nw is number of interlacing points weft cover on warp which is related to the total number of weft yarns (Nw) and the basic structure of the fabric. For example, as \(\frac{1}{ 1}\) plain weave, the number of weft yarns in base structure is 2, interlacing point is 1, \(n_{{\text{w}}} = \frac{{N_{{\text{w}}} }}{2} \times 1\); \({\text{as }}\;\frac{1}{ 2} \nwarrow\) twill weave, the number of weft yarns in base structure is 3, interlacing points is 1, \(n_{{\text{w}}} = \frac{{N_{{\text{w}}} }}{3} \times 1\).

Fig. 3
figure3

Schematic diagram of a resistance measurement on warp direction, b circuit diagram, c equivalent resistance of whole resistance on warp direction

Accordingly, the resistance of woven fabric on weft direction (Rw) can be expressed as

$$R_{{\text{w}}} = \frac{{R_{{{\text{aw}}}} }}{{N_{{\text{w}}} }} + \frac{{R_{{\text{cj}}} + R_{{{\text{aj}}}} }}{{n_{{\text{j}}} }}$$
(7)

where Nw is the total number of weft yarns; nj is number of points warp interwoven with weft; and Rcj is the contact resistance of each interlacing point, where current flows through warp yarn to weft according to Eq. (4).

According to Eqs. (6) and (7), the resistance of woven fabric is related to axial resistance of yarn (Raj, Raw), the contact resistance of the yarn (Rcj, Rcw), the density of the yarn arrangement (Nj, Nw), and the number of interweaving points (nj, nw), by increasing the yarn arrangement density and number of interlacing points or decreasing the contact resistance and axial resistance of yarn which can reduce the resistance of the woven fabric.

The sensing performance of woven fabric strain sensor on uniaxial stretching

Woven fabrics are made of interwoven warp and weft yarns, when the fabric is subjected to uniaxial stretching; the different strains on warp or weft direction will occur due to different interactions (friction, shear) between the warp and weft yarns. These strains include quick-elastic strain that can be recovered immediately, time-dependent slow-elastic strain and non-recoverable plastic strain. The latter two factors are the main causes of hysteresis of fabric sensors [2, 25]. Therefore, the rapid elastic strain range is an ideal working area for fabric sensors. For the sake of research, the following assumptions are made: (1) The section of yarn remains circular and volume remains unchanged during stretching. (2) The yarn structure is uniform, strain is within the elastic strain range of the fabric (stretching below the yield stress), and the fabric did not arch or fold.

When the fabric is subjected to uniaxial stretching (if on warp direction), two different stages of strain will be occurred: on first stage, the geometrical structure of woven fabric changes and the necking phenomenon occurs, that is shrinkage of warp and weft yarns changes, while the warp and weft yarns diameters remain unchanged (as shown in Fig. 4a). On second stage, the warp shrinkage reaches the minimum value (\(\theta_{{\text{j}}} \to 0)\) and the weft shrinkage reaches the maximum value (\(\theta_{{\text{w}}} \to \pi )\) (as shown in Fig. 4b, c); further stretching on warp direction, the warp yarn is deformed, while the deformation of weft is very small because of maximum shrinkage and the tight structure of fabric on weft direction [26, 27].

Fig. 4
figure4

Schematic diagram of fabric uniaxial stretching on Stage I a extension on warp direction and necking contraction on weft direction, b initial state (cj = cj0, cw = cw0), c the final state of Stage I (\(c_{{\text{j}}} \to 0,c_{{\text{w}}} \to \hbox{max}\))

The sensitivity of woven fabric sensor can be expressed as:

$${\text{GF}} = \frac{dR}{{R_{0} \varepsilon }}$$
(8)

where \(\frac{dR}{{R_{0} }}\) is the rate of resistance change on applied force; ε is the strain.

The sensing performance caused by fabric geometry structure change (Stage I)

In order to study the relationship between structure and electro-mechanical properties of fabric, Peirce geometric model (PGM) of woven fabric is introduced as shown in Fig. 5. There are some mathematical equations between fabric structural parameters according to PGM as follows [28]:

$$h_{{\text{j}}} + h_{{\text{w}}} = D_{{\text{j}}} + D_{{\text{w}}}$$
(9)
$$\frac{{h_{{\text{j}}} }}{{\alpha_{{\text{w}}} }} = \frac{4}{3}\sqrt {c_{{\text{j}}} } ;\quad \frac{{h_{{\text{w}}} }}{{\alpha_{{\text{j}}} }} = \frac{4}{3}\sqrt {c_{{\text{w}}} }$$
(10)
$$\theta_{{\text{j}}} = 212\sqrt {c_{{\text{j}}} } ;\quad \theta_{{\text{w}}} = 212\sqrt {c_{{\text{w}}} }$$
(11)
$$c_{{\text{j}}} = \frac{{L_{{\text{j}}} }}{A} - 1 = \frac{{l_{{\text{j}}} }}{{\alpha_{{\text{w}}} }} - 1; \quad c_{{\text{w}}} = \frac{{L_{{\text{w}}} }}{B} - 1 = \frac{{l_{{\text{w}}} }}{{\alpha_{{\text{j}}} }} - 1$$
(12)
$$l_{{\text{j}}} = \frac{{L_{{\text{j}}} }}{{N_{{\text{w}}} }}; \quad l_{{\text{w}}} = \frac{{L_{{\text{w}}} }}{{N_{{\text{j}}} }}$$
(13)
$$\alpha_{{\text{w}}} = \frac{A}{{N_{{\text{j}}} }} = \frac{{l_{{\text{j}}} }}{{1 + c_{{\text{j}}} }} = \frac{{L_{{\text{j}}} }}{{N_{{\text{w}}} }}\frac{1}{{1 + c_{{\text{j}}} }}; \quad \alpha_{{\text{j}}} = \frac{B}{{N_{{\text{w}}} }} = \frac{{l_{{\text{w}}} }}{{1 + c_{{\text{w}}} }} = \frac{{L_{{\text{w}}} }}{{N_{{\text{j}}} }}\frac{1}{{1 + c_{{\text{w}}} }}$$
(14)

where αw and αj are the spacing between the adjacent weft or warp; cj and cw are the warp and weft shrinkage of fabric; hj and hw are the crimp wave heights of warp or weft; lj and lw are the crimp wave lengths of warp or weft; Lj and Lw are the lengths of warp or weft; Nj and Nw are the numbers of warp or weft; θj and θw are the contact angles of warp cover on weft or weft cover on warp; A is the length of the fabric; and B is the width of the fabric.

Fig. 5
figure5

Peirce geometric model of woven fabric

In Stage I, only the structure of fabric changes and no deformation occurs on warp or weft yarns; so the following equations can set up:

$$dL_{{\text{j}}} = d\frac{{L_{{\text{j}}} }}{{N_{{\text{j}}} }} = dl_{{\text{j}}} = 0;\quad dl_{{\text{w}}} = d\frac{{L_{{\text{j}}} }}{{N_{{\text{w}}} }} = dl_{{\text{w}}} = 0$$
(15)
$$dR_{{{\text{aj}}}} = 0; \quad dR_{{{\text{aw}}}} = 0$$
(16)
$$d\left( {D_{{\text{w}}} + D_{{\text{j}}} } \right) = d\left( {h_{{\text{j}}} + h_{{\text{w}}} } \right) = 0$$
(17)

According to Eqs. (12), (13), (14), and (15)

$$dl_{{\text{j}}} = (1 + c_{{\text{j}}} )d\alpha_{{\text{w}}} + \alpha_{{\text{w}}} dc_{{\text{j}}} = 0;\quad dl_{{\text{w}}} = \left( {1 + c_{{\text{w}}} } \right)d\alpha_{{\text{j}}} + \alpha_{{\text{j}}} dc_{{\text{w}}} = 0$$
(18)
$$\frac{{d\alpha_{{\text{w}}} }}{{a_{{\text{w}}} }} = \varepsilon_{{\text{j}}} ; \quad \frac{{d\alpha_{{\text{j}}} }}{{a_{{\text{j}}} }} = \varepsilon_{{\text{w}}}$$
(19)
$$dc_{{\text{j}}} = - \left( {1 + c_{{\text{j}}} } \right)\varepsilon_{{\text{j}}}$$
(20)
$$dc_{{\text{w}}} = - \left( {1 + c_{{\text{w}}} } \right)\varepsilon_{{\text{w}}}$$
(21)
$$\alpha_{{\text{w}}} = \alpha_{{\text{w}}0} \left( {1 + \varepsilon_{{\text{j}}} } \right); \quad \alpha_{{\text{w}}} = \frac{{l_{{\text{j}}} }}{{\left( {1 + c_{{\text{j}}} } \right)}}; \quad \alpha_{{\text{w}}0} = \frac{{l_{{\text{j}}} }}{{\left( {1 + c_{{\rm j}0} } \right)}}$$
(22)

Rearranging Eq. (22), we get

$$\varepsilon_{{\text{j}}} = \frac{{c_{{\rm j}0} - c_{{\text{j}}} }}{{c_{{\text{j}}} + 1}}\quad (\because\,c_{{\rm j}0} > c_{{\text{j}}} , \therefore \,\varepsilon_{{\text{j}}} > 0)$$
(23)

Similarly

$$\varepsilon_{{\text{w}}} = - \frac{{c_{{\text{w}}} - c_{{\text{w}}0} }}{{c_{{\text{w}}} + 1}}\quad (\because\,c_{{\text{w}}0} < c_{{\text{w}}} , \therefore\, \varepsilon_{{\text{w}}} < 0)$$
(24)
$$\frac{{\varepsilon_{{\text{w}}} }}{{\varepsilon_{{\text{j}}} }} = - \frac{{\left( {c_{{\text{w}}} - c_{{\text{w}}0} } \right)\left( {c_{{\text{j}}} + 1} \right)}}{{\left( {c_{{\text{w}}} + 1} \right)\left( {c_{{\rm j}0} - c_{{\text{j}}} } \right)}}$$
(25)

where εj and εw are the strains of fabric on warp or weft direction; cj0 and cw0 are the initial shrinkage of warp or weft. \(\alpha_{{\text{w}}0}\) is the initial spacing between the adjacent wefts.

When there is uniaxial stretching on warp direction, the resistance change rate of the warp system (Rj) can be expressed as:

$$R_{{{\text{aj}}}} = 4\rho_{\text{a}} \frac{{L_{{\text{j}}} }}{{\pi D_{{\text{j}}}^{2} }} = {\text{const}};\quad R_{{\text{cw}}} = \frac{{\rho_{\text{r}} }}{{D_{{\text{w}}} \theta_{{\text{w}}} }} = \frac{{\rho_{\text{r}} }}{{212D_{{\text{w}}} \sqrt {c_{{\text{w}}} } }}$$
(26)
$$dR_{{\text{j}}} = \frac{1}{{n_{{\text{w}}} }}dR_{{\text{cw}}}$$
(27)

According to Eqs. (5) and (11)

$$dR_{{\text{cw}}} = d\frac{{\rho_{\text{r}} }}{{212D_{{\text{w}}} \sqrt {c_{{\text{w}}} } }} = - \frac{1}{2} \times \frac{{\rho_{\text{r}} }}{{212D_{{\text{w}}} }}c_{{\text{w}}}^{ - 3/2} dc_{{\text{w}}} = - \frac{{R_{{\text{cw}}} }}{{2c_{{\text{w}}} }}dc_{{\text{w}}}$$
(28)

Rearranging Eqs. (21), (27), and (28), we get:

$$dR_{{\text{j}}} = \frac{1}{{n_{{\text{w}}} }}R_{{\text{cw}}} \frac{{1 + c_{{\text{w}}} }}{{2c_{{\text{w}}} }}\varepsilon_{{\text{w}}}$$
(29)

According to Eqs. (5) and (6), the initial resistance on warp direction of fabric (\(R_{{\rm j}0}\)) and initial contacted Rcw0 can be expressed as:

$$R_{{\rm j}0} = \frac{{R_{{{\text{aj}}}} }}{{N_{{\text{j}}} }} + \frac{{R_{{\text{cw}}0} + R_{{{\text{aw}}}} }}{{n_{{\text{w}}} }};\quad R_{{\text{cw}}0} = \frac{{\rho_{\text{r}} }}{{D_{{\text{w}}} \theta_{{\text{w}}0} }} = \frac{{\rho_{\text{r}} }}{{212D_{{\text{w}}} \sqrt {c_{{\text{w}}0} } }}$$
(30)
$$\frac{{dR_{{\text{j}}} }}{{R_{{\rm j}0} }} = \frac{{R_{{\text{cw}}} }}{{\frac{{n_{{\text{w}}} }}{{N_{{\text{j}}} }}R_{{{\text{aj}}}} + R_{{\text{cw}}0} + R_{{{\text{aw}}}} }}\frac{{1 + c_{{\text{w}}} }}{{2c_{{\text{w}}} }}\varepsilon_{{\text{w}}} = \frac{{\frac{{\rho_{\text{r}} }}{{212D_{{\text{w}}} \sqrt {c_{{\text{w}}} } }}}}{{\frac{{n_{{\text{w}}} }}{{N_{{\text{j}}} }}4\rho_{\text{a}} \frac{{L_{{\text{j}}} }}{{\pi D_{{\text{j}}}^{2} }} + \frac{{\rho_{\text{r}} }}{{212D_{{\text{w}}} \sqrt {c_{{\text{w}}0} } }} + 4\rho_{\text{a}} \frac{{L_{{\text{w}}} }}{{\pi D_{{\text{w}}}^{2} }}}}\frac{{1 + c_{{\text{w}}} }}{{2c_{{\text{w}}} }}\varepsilon_{{\text{w}} }$$
(31)

Rearranging (25), (30), and (31), the resistance change rate on Stage I \(\left( {\frac{{dR_{{\text{j}}} }}{{R_{{\rm j}0} }}} \right)_{1}\) can be expressed as

$$\left( {\frac{{dR_{{\text{j}}} }}{{R_{{\rm j}0} }}} \right)_{1} = - \frac{{\left( {c_{{\text{w}}} - c_{{\text{w}}0} } \right)\left( {c_{{\text{j}}} + 1} \right)}}{{2c_{{\text{w}}} \left( {c_{{\text{j}}0} - c_{{\text{j}}} } \right)}}\frac{{\frac{{\rho_{\text{r}} }}{{212D_{{\text{w}}} \sqrt {c_{{\text{w}}} } }}}}{{\frac{{n_{{\text{w}}} }}{{N_{{\text{j}}} }}4\rho_{\text{a}} \frac{{L_{{\text{j}}} }}{{\pi D_{{\text{j}}}^{2} }} + \frac{{\rho_{\text{r}} }}{{212D_{{\text{w}}} \sqrt {c_{{\text{w}}0} } }} + 4\rho_{\text{a}} \frac{{L_{{\text{w}}} }}{{\pi D_{{\text{w}}}^{2} }}}}\varepsilon_{{\text{j}}}$$
(32)

The sensitivity of woven fabric sensor on warp direction at Stage I (\({\text{GF}}_{\text{j}1} )\) can be expressed as:

$${\text{GF}}_{\text{j}1} = - \frac{{\left( {c_{{\text{w}}} - c_{{\text{w}}0} } \right)\left( {c_{{\text{j}}} + 1} \right)}}{{2c_{{\text{w}}} \left( {c_{{\text{j}}0} - c_{{\text{j}}} } \right)}}\frac{{\frac{{\rho_{\text{r}} }}{{212D_{{\text{w}}} \sqrt {c_{{\text{w}}} } }}}}{{\frac{{n_{{\text{w}}} }}{{N_{{\text{j}}} }}4\rho_{\text{a}} \frac{{L_{{\text{j}}} }}{{\pi D_{{\text{j}}}^{2} }} + \frac{{\rho_{\text{r}} }}{{212D_{{\text{w}}} \sqrt {c_{{\text{w}}0} } }} + 4\rho_{\text{a}} \frac{{L_{{\text{w}}} }}{{\pi D_{{\text{w}}}^{2} }}}}$$
(33)

It can be known from the analysis of Eq. (33) as follow:

  1. 1.

    When stretching on warp direction, the GFj1 is negative correlation with strain on warp direction (εj).

  2. 2.

    GFj1 is related to the shrinkage of fabric on warp or weft direction (\(c_{{\text{j}}} ,c_{{\text{w}}} )\), since GFj1 is not constant, so the sensitivity of fabric sensors whatever on warp or weft direction is nonlinear at the Stage I.

  3. 3.

    Increasing the shrinkage of warp yarns (cj) and the number of warp yarns (Nj), or decreasing the shrinkage of weft yarns (cw) and the number of interweaving, points (nw) can improve the sensitivity of the fabric sensor. For example, twill weave is with relatively few interweave points (nw) than plain weave; the sensitivity of twill woven fabric strain sensor is higher than plain woven.

The sensing performance caused by deformation of yarn (Stage II)

On second stage, when \(\varepsilon_{{\text{j}}} > \varepsilon_{\text{jc}}\)(\(\varepsilon_{\text{jc}}\) is the critical strain when cj = 0), the contact resistance Rcj tends to infinity, which means no currents flow through warp to weft and the resistance of fabric on weft direction (Rw) is \(\frac{{R_{{{\text{aw}}}} }}{{N_{{\text{w}}} }}\). Meanwhile the shrinkage of weft (cw) and the contact angle where weft cover on warp (\(\theta_{{\text{w}}} )\) tends to maximum value \((c_{\text{wmax} } , \theta_{\text{wmax} } ,\) Fig. 4c) and the contact resistance Rcw tends to the minimum value \(R_{\text{cwmin} } = \frac{{\rho_{\text{r}} }}{{212\sqrt {c_{\text{wmax} } } D_{{\text{w}}} }}\). So the resistance of fabric on warp direction (Rj) is \(\frac{{R_{{{\text{aj}}}} }}{{N_{{\text{j}}} }} + \frac{{R_{\text{cwmin} } + R_{{{\text{aw}}}} }}{{n_{{\text{w}}} }}\). Under the condition of small strain, when the warp is stretched, the force on weft yarn is very small and its deformation can be ignored [26]. The resistance change of fabric on warp direction can be expressed as

$$dR_{{\text{j}}} = \frac{{dR_{{{\text{aj}}}} }}{{N_{{\text{j}}} }}\quad (\because\,R_{\text{cwmin} } \approx {\text{const}}, \, R_{{{\text{aw}}}} \approx {\text{const}})$$
(34)

As shown in Fig. 6 according to the assumption (1) that the yarn has no volume change at small strain, the following equation can be derived:

$$\frac{1}{4}\pi D_{{\text{j}}0}^{2} L_{{\text{j}}0} = \frac{1}{4}\pi D_{{\text{j}}}^{2} L_{{\text{j}}} ;\quad \frac{{L_{{\text{j}}} }}{{L_{{\text{j}}0} }} = \left( {\frac{{D_{{\text{j}}0} }}{{D_{{\text{j}}} }}} \right)^{2} ;\quad \frac{{L_{{\text{j}}} }}{{L_{{\text{j}}0} }} = \varepsilon_{y} + 1; \quad \frac{{D_{{\text{j}}0} }}{{D_{{\text{j}}} }} = \frac{1}{{\varepsilon_{x} + 1}}$$
(35)
$$\varepsilon_{x} + 1 = \frac{{\sqrt {\varepsilon_{y} + 1} }}{{\varepsilon_{y} + 1}};\quad \sqrt {\varepsilon_{y} + 1} - 1 \approx \frac{{\varepsilon_{y} }}{2}; \quad \varepsilon_{x} \approx - \frac{{\varepsilon_{y} }}{{2\left( {\varepsilon_{y} + 1} \right)}}$$
(36)
Fig. 6
figure6

Schematic diagram of radial and axial strain of yarn (\(\varepsilon_{y} ,\varepsilon_{x}\)) on Stage II

And according to surface specific resistance formula of uniform materials

$$R = \rho \frac{{L_{{\text{j}}} }}{S};\quad dR = \rho d\frac{{L_{{\text{j}}} }}{S} = \rho \frac{{SdL_{{\text{j}}} - L_{{\text{j}}} dS}}{{S^{2} }} = \rho \frac{{dL_{{\text{j}}} }}{S} - \rho \frac{dS}{{S^{2} }} = R\frac{{dL_{{\text{j}}} }}{{L_{{\text{j}}} }} - R\frac{dS}{S}$$
(37)
$$S = \frac{{\pi D_{{\text{j}}}^{2} }}{4};\quad dS = \frac{{\pi D_{{\text{j}}} dD_{{\text{j}}} }}{2};\quad \frac{dS}{S} = 2\frac{{dD_{{\text{j}}} }}{{D_{{\text{j}}} }} = 2\varepsilon_{x} \frac{{dD_{{\text{j}}} }}{{D_{{\text{j}}} }} = \varepsilon_{x} \frac{{dL_{{\text{j}}} }}{{L_{{\text{j}}} }} = \varepsilon_{y}$$
(38)
$$dR = R\left( {\frac{{dL_{{\text{j}}} }}{{L_{{\text{j}}} }} - \frac{dS}{S}} \right) = R(\varepsilon_{y} - 2\varepsilon_{x} ) \approx R\frac{{\varepsilon_{y} \left( {\varepsilon_{y} + 2} \right)}}{{\varepsilon_{y} + 1}}$$
(39)
$$\frac{R}{{R_{0} }} = \frac{{\rho \frac{{L_{{\text{j}}} }}{S}}}{{\rho \frac{{L_{{\text{j}}0} }}{{S_{0} }}}} = \frac{{LS_{0} }}{{L_{0} S}} = \frac{{\frac{1}{4}\pi D_{{\text{j}}0}^{2} L_{{\text{j}}} }}{{\frac{1}{4}\pi D_{{\text{j}}}^{2} L_{{\text{j}}0} }} = \left( {\frac{{L_{{\text{j}}} }}{{L_{{\text{j}}0} }}} \right)^{2} = (\varepsilon_{y} + 1)^{2}$$
(40)

where \(\varepsilon_{x ,} \varepsilon_{y}\) are the strains of yarn on radial and axial direction; Dj0, Dj Lj0, Lj, S0, and S are the diameter, length and section area of yarn at initial state or under stretching.

Rearranging (39) and (40), we get

$$dR \approx R_{0} \varepsilon_{y} \left( {\varepsilon_{y} + 1} \right)\left( {\varepsilon_{y} + 2} \right)$$
(41)
$$dR_{{\text{j}}} = \frac{{dR_{{{\text{aj}}}} }}{{N_{{\text{j}}} }} = \frac{{R_{{{\text{a}}j0}} }}{{N_{{\text{j}}} }}\varepsilon_{y} \left( {\varepsilon_{y} + 1} \right)\left( {\varepsilon_{y} + 2} \right)$$
(42)
$$\left( {\frac{{dR_{{\text{j}}} }}{{R_{{\text{j}}0} }}} \right)_{2} = \frac{{R_{{{\text{a}}j0}} }}{{R_{{{\text{a}}j0}} + N_{{\text{j}}} \frac{{R_{\text{cwmin} } + R_{{{\text{a}}w0}} }}{{n_{{\text{w}}} }}}}\varepsilon_{y} \left( {\varepsilon_{y} + 1} \right)\left( {\varepsilon_{y} + 2} \right)$$
(43)

where \(\left( {\frac{{dR_{{\text{j}}} }}{{R_{{\text{j}}0} }}} \right)_{2}\) is the change rate of warp direction resistance on Stage II.

Considering the assumption of the elastic strain of the yarn, the range of \(\varepsilon_{y}\) is small, so the higher power of \(\varepsilon_{y}\) can be skipped; Eq. (43) can be expressed as:

$$\left( {\frac{{dR_{{\text{j}}} }}{{R_{{\text{j}}0} }}} \right)_{2} \approx \frac{{2R_{{{\text{a}}j0}} }}{{R_{{{\text{a}}j0}} + N_{{\text{j}}} \frac{{R_{\text{cwmin} } + R_{{{\text{a}}w0}} }}{{n_{{\text{w}}} }}}}\varepsilon_{y}$$
(44)

Considering the strain already occurred in the first stage, the strain occurred in the second stage should be removed from the strain in the first stage that is

$$\varepsilon_{y} = \varepsilon_{{\text{j}}} - \varepsilon_{\text{jc}}$$
(45)
$${\text{GF}}_{\text{j}2} \approx \frac{{2R_{{{\text{a}}j0}} }}{{R_{{{\text{a}}j0}} + N_{{\text{j}}} \frac{{R_{\text{cwmin} } + R_{{{\text{a}}w0}} }}{{n_{{\text{w}}} }}}}\left( {1 - \frac{{\varepsilon_{\text{jc}} }}{{\varepsilon_{{\text{j}}} }}} \right)$$
(46)

where \(\varepsilon_{\text{jc}}\) is critical strain when cj = 0; \({\text{GF}}_{\text{j}2}\) is the sensitivity on warp direction of woven fabric at Stage II.

It can be known from the analysis of Eqs. (44), (45), and (46):

  1. 1.

    GFj2 can be improved by increasing the interweaving points of warp and weft (nw), increasing the initial resistance of warp (Rcj0), or decreasing the initial resistance (Raw0) and the minimum contact resistance of weft (Rcwmin), as well as the number of warp yarns (Nj).

  2. 2.

    GFj2 values are approximately linear with the strain occurred on stage II (εy) but nonlinear with the whole strain of the fabric (εj).

Experimental verification

Two different fabric structures (twill and plain weave) were prepared for the comparison and verification of its sensing performance experimentally. The theoretical value of \({c}_{{\mathbf{j0}}} ,{c}_{{\mathbf{w0}}} ,{c}_{{\mathbf{j}}} ,{c}_{{\mathbf{w}}}\), \(R_{{\text{cw}}}\), \(\left( {\frac{{dR_{{\text{j}}} }}{{R_{{\text{j}}0} }}} \right)_{1} \left( {\frac{{dR_{{\text{j}}} }}{{R_{{\text{j}}0} }}} \right)_{2} ,{\text{GF}}_{\text{j}1} ,{\text{GF}}_{\text{j}2}\) can be derived by relevant equation and is listed in Tables 1 and 2. As shown in Fig. 7, the experimental measurement curve of \(\frac{{dR_{{\text{j}}} }}{{R_{{\text{j}}0} }}\sim\varepsilon_{{\text{j}}}\) and GFj are basically consistent with the value obtain by Eqs. (32), (33), (44), and (46), which prove the credibility of theoretical results derived by Pierce geometry model of fabric and assumption of elastic strain of yarn. In addition, the sensitivity of the strain sensor based on woven fabric structure is relatively small (|GFj| < 2) no matter theoretical derivation or experimental verification. At the first stage, the change of resistance is negatively correlated with strain (strain increases and resistance decreases), while in the second stage, the change of resistance is positively correlated with strain (strain increases and resistance increases). After the second stage of stretching, the plastic deformation may be caused by the fabric structure damage (staple slipping, fabric folding etc.), resulting in the fluctuation of the resistance value and the instability of the sensing performance; therefore, it should not be included in the reliable working strain range of the fabric strain sensor. It is necessary to note that the small GF value of our results are probably due to the electrical conductive plied yarns to weave fabric sensor in our experiment was made of continuous entangled and twisted conductive staple yarns with large aspect ratio, its connection-disconection state between the fibers is less changed. Therefore the sensitivity of our woven fabric sensor is affected mainly by the geometric effect sensing mechanism, secondary by the connection-disconnect sensing mechanism as it does in the case of coating graphene on the surface of fabric which often exhibits high sensitivity [5, 29]. Finally, what needs further explanation is that different fabric structures exhibit different GF values and resistance change rate (Fig. 8a, b); twill weave normally has a larger resistance change rate and GF value than plain weave mainly because twill weave is prone to deformation during stretching and its current path is less than plain weave.

Table 1 The calculated values of fabric structure and electrical properties (twill weave)
Table 2 The calculated values of fabric structure and electrical properties (plain weave)
Fig. 7
figure7

Experimental curve and the calculated value derived by the theoretical formula a dRj/Rj − εj of twill weave, b dRj/Rj − εj of plain weave, c GFj − εj of twill weave, d GFj − εj of plain weave

Fig. 8
figure8

Comparison experimental curve of different fabric structures (plain, twill weave). a dRj/Rj − εj curve, b GFj − εj curve

Conclusion

Based on the fabric geometry model of Pierce and the assumption of elastic strain of yarn, the relationship between the parameters of 3D network structure of woven fabric strain sensor and its sensing performance on uniaxial stretching was studied and the mathematical relationship was derived; these theoretical conclusions were verified by uniaxial stretching experiment. It can be found that the sensitivity was relatively small and nonlinear if only geometric effect sensing mechanism works. In order to improve the sensitivity and linearity of woven fabric strain sensor on warp direction, in addition to adjusting the structural parameters of the fabric (Nj, nw, cw), other sensing mechanisms, such as connection disconnection effect and piezoresistive effect, should be adopted.

References

  1. 1.

    Lina MC, Alison BF (2014) Smart fabric sensors and e-textile technologies: a review. Smart Mater Struct 23:053001

  2. 2.

    Seyedin S, Zhang P, Naebe M, Qin S, Chen J, Wang X, Razal JM (2019) Textile strain sensors: a review of the fabrication technologies, performance evaluation and applications. Mater Horiz 6:219–249

  3. 3.

    Hughes-Riley T, Dias T, Cork C (2018) A historical review of the development of electronic textiles. Fibers 6:34–38

  4. 4.

    Persson NK, Martinez JG, Zhong Y, Maziz A, Jager EWH (2018) Actuating textiles: next generation of smart textiles. Adv Mater Technol 1700397:1–12

  5. 5.

    Morteza A, Ki-UK K, Inkyu P, Metin S (2016) Stretchable, skin-mountable, and wearable strain sensors and their potential applications: a review. Adv Funct Mater 26:1678–1698

  6. 6.

    Kyeong NK, Chun J, Jin WK, Lee KY, Jang-Ung P, SangWoo K, Wang ZL, Jeong MB (2015) Highly stretchable 2D fabrics for wearable triboelectric nanogenerator under harsh environments. ACS Nano 9:6394–6400

  7. 7.

    Lee S, Ko W, Oh Y, Lee J, Baek G, Lee Y, Sohn J, Cha S, Kim J, Park J (2015) Triboelectric energy harvester based on wearable textile platforms employing various surface morphologies. Nano Energy 12:410–418

  8. 8.

    Liu L, Pan J, Chen P, Zhang J, Yu X, Ding X, Wang B, Sun X, Peng H (2014) A triboelectric textile templated by a three-dimensionally penetrated fabric. J Mater Chem A 4:6077–6083

  9. 9.

    Pu X, Li L, Liu M, Jiang C, Du C, Zhao Z, Xu W, Wang ZL (2016) Wearable self-charging power textile based on flexible yarn supercapacitors and fabric nanogenerators. Adv Mater 28:98–105

  10. 10.

    Yu X, Pan J, Deng J, Zhou J, Sun X, Peng H (2016) A novel photoelectric conversion yarn by integrating photomechanical actuation and the electrostatic effect. Adv Mater 28:10744–10749

  11. 11.

    Hu N, Itoi T, Akagi T, Kojima T, Xue J, Yan C, Atobe S, Fukunaga H, Yuan W, Ning H, Surina Liu Y, Alamusi (2013) Ultrasensitive strain sensors made from metal-coated carbon nanofiller/epoxy composites. Carbon 51:202–212

  12. 12.

    Heo JS, Eom J, Kim YH, Park SK (2017) Recent progress of textile-based wearable electronics: a comprehensive review of materials, devices, and applications. Small 1703034:1–16

  13. 13.

    Nag A, Mukhopadhyay SC, Kosel J (2017) Wearable flexible sensors: a review. IEEE Sens J 17:3949–3960

  14. 14.

    Wang C, Li X, Gao E, Jian M, Xia K, Wang Q, Xu Z, Ren T, Zhang Y (2016) Carbonized silk fabric for ultrastretchable, highly sensitive, and wearable strain sensors. Adv Mater 28:6640–6648

  15. 15.

    Du DH, Li PC, Ouyang J (2013) Graphene coated nonwoven fabrics as wearable sensors. J Mater Chem C 00(1–3):1–9

  16. 16.

    Foroughi J, Spinks GM, Aziz S, Mirabedini A, Jeiranikhameneh A, Wallace GG, Kozlov ME, Baughman RH (2016) Knitted carbon-nanotube-sheath/spandex-core elastomeric yarns for artificial muscles and strain sensing. ACS Nano 10:9129–9135

  17. 17.

    Chou S, Chen HE (1995) The weaving methods of three-dimensional fabrics of advanced composite materials. Compos Struct 33:159–172

  18. 18.

    Seyedin S, Razal JM, Innis PC, Jeiranikhameneh A, Beirne S, Wallace GG (2015) Knitted strain sensor textiles of highly conductive all-polymeric fibers. ACS Appl Mater Interfaces 7:21150–21158

  19. 19.

    Yan T, Wang Z, Pan ZJ (2018) A highly sensitive strain sensor based on a carbonized polyacrylonitrile nanofiber woven fabric. J Mater Sci 53:11917–11931

  20. 20.

    Ge J, Sun L, Zhang FR, Zhang Y, Shi L, Zhao HW, Jiang HL, Yu SH (2016) A stretchable electronic fabric artificial skin with pressure, lateral strain and flexion-sensitive properties. Adv Mater 28:722–728

  21. 21.

    Wang Y, Wang L, Yang T, Li X, Zang X, Zhu M, Wang K, Wu D, Zhu H (2014) Wearable and highly sensitive graphene strain sensors for human motion monitoring. Adv Funct Mater 24:4666–4670

  22. 22.

    Pang C, Koo JH, Nguyen A, Caves JM, Kim MG, Chortos A, Kim K, Wang PL, Tok JB, Bao Z (2014) Highly skin-conformal microhairy sensor for pulse signal amplification. Adv Mater 27:634–640

  23. 23.

    Ma H, Wu W, Cao J, Yue B, Zhang H (2017) Network structure and electromechanical properties of viscose-graphene conductive yarn assembles. Carbon 114:731–739

  24. 24.

    Realff ML, Boyce MC, Backer S (1997) A micromechanical model of the tensile behavior of woven fabric. Text Res J 67:445–459

  25. 25.

    Shyr TW, Shie JW, Jhuang YE (2011) The effect of tensile hysteresis and contact resistance on the performance of strain-resistant elastic-conductive webbing. Sensors 11(2):1693–1705

  26. 26.

    Peirce FT (1928) The influence of humidity on the elastic properties of starch film. J Text Inst Trans T28:228–252

  27. 27.

    Leaf GAV (2004) The mechanics of plain woven fabrics. Int J Cloth Sci Technol 16:97–107

  28. 28.

    Jeon BS, Chun SY, Hong CJ (2003) Structural and mechanical properties of woven fabrics employing Peirce’s model. Text Res J 73:929–933

  29. 29.

    Li X, Zhang R, Yu W, Wang K, Wei J, Wu D, Gao A, Li Z, Cheng Y, Zheng Q, Ruoff RS, Zhu H (2012) Stretchable and highly sensitive graphene-on-polymer strain sensors. Sci Rep (UK) 2:870

Download references

Acknowledgements

The work was financially supported by the Public Technology Research Plan of Zhejiang Province (LGF18E030003), National Natural Science Foundation of China (51672251), and 521 Talent Project of Zhejiang Sci-Tech University.

Author information

Correspondence to Juming Yao.

Ethics declarations

Conflict of interest

The authors declare that they have no conflict of interest.

Additional information

Publisher's Note

Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.

Electronic supplementary material

Below is the link to the electronic supplementary material.

Supplementary material 1 (DOCX 725 kb)

Rights and permissions

Reprints and Permissions

About this article

Verify currency and authenticity via CrossMark

Cite this article

Liu, Y., Liu, L., Li, Z. et al. 3D network structure and sensing performance of woven fabric as promising flexible strain sensor. SN Appl. Sci. 2, 70 (2020) doi:10.1007/s42452-019-1857-6

Download citation

Keywords

  • Strain sensor
  • Woven fabric
  • Pierce’s fabric geometry model
  • Elastic strain