\r\n\tHence, this book is targeted to deliver the bundled characteristics and features of MXenes to transfer the various scopes and virtues to the research community.
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His research interests are centered around the cost-effective fabrication of low-dimensional materials for electronics and energy devices. He has authored more than 175 international peer-reviewed research articles and numerous various forms of research publications.",coeditorOneBiosketch:null,coeditorTwoBiosketch:null,coeditorThreeBiosketch:null,coeditorFourBiosketch:null,coeditorFiveBiosketch:null,editors:[{id:"199404",title:"Prof.",name:"Dhanasekaran",middleName:null,surname:"Vikraman",slug:"dhanasekaran-vikraman",fullName:"Dhanasekaran Vikraman",profilePictureURL:"https://mts.intechopen.com/storage/users/199404/images/system/199404.png",biography:"Dr. Dhanasekaran Vikraman is an assistant professor in the Division of Electronics and Electrical Engineering, Dongguk University, Seoul, Korea. He received his bachelor’s degree from Mannai Rajagopalaswamy Government Arts College, Mannargudi, affiliated with Bharathidasan University, India. He completed his master’s degree and Ph.D. at the Department of Physics, Alagappa University, India. Later, he received a visiting scientist position at KIST, Korea; a Marie-Curie Experienced Researcher fellowship at the Department of Physics, Aristotle University of Thessaloniki, Greece; and post-doc positions at Sejong University and Ajou University, Korea. He has authored more than 180 international journal articles and 3 book chapters and edited several books. 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1. Introduction
Most of the methods for environment abstraction from multiple views are just relying on points and ignoring other basic shapes like lines. Line based Structure from Motion methods based on lines create an abstraction based on straight line segments from a set of images. Analogously to point based abstraction methods like SIFT, in order to estimate the three-dimensional coordinates of lines in an spatial representation, the correspondences between lines among multiple images must be obtained by using detection and matching. The matching process for lines across the different views will return correspondences that can be exploited using 3D geometric relations. The matched features (points or lines) among views are used to estimate the position of cameras, referred to as extrinsic parameters. From the camera poses, the features are forward projected in the 3D abstraction or sketch.
The 3D line abstraction methods based on straight line segments that are most frequently found in the literature are designed to work altogether with detailed point-based reconstructions [1], therefore employing the camera extrinsic parameters obtained from these point rotation and translation invariants. This permits higher accuracy in the 3D reconstructions than using solely straight lines. A different approach employs only straight line segment correspondences in the reconstruction, independently of point based 3D reconstructions [2]. This approach has been proved advantageous over the first one in scenarios where not enought feature points can be accurately put in correspondence between the different views. There are few publications about uncertainty analysis in 3D line reconstructions based on lines. One of the most recent ones explains the state of the art for these metrics [3].
Oppositely to points, straight lines have a direction, and this dimensionality can be exploited geometrically. The intersection of coplanar straight lines reveal geometrical information. Likewise, groups of segments will also indicate the location of the most probable vanishing points from a camera plane [4]. These geometric properties are not offered by points, therefore lines can be a good complement when performing a spatial reconstruction [5, 6]. Additionally, pairs of straight line segments are often related by the strong constraints of parallelism and orthogonality [7, 8]. This allows to combine individual similarities of pairs of segments altogether with the coplanarity constraints [9]. A recent work employed 3D lines to reconstruct surfaces [10].
1.1 SfM lines carry higher complexity
In literature, research about straight segments have always been developed after works related to feature points. Lines have often been left as a complement for applications of these works devoted to feature points. There are reasons for the line based SfM to be more complex than a feature point based one:
Detection of points is restrained to sole coordinates in images, while line detection extends to several pixels that are ideally adjacent to other pixels of the line. Nevertheless, in practice, detecting the limits of a straight line segment is not trivial in real images, due to digital noise, occlusions or changes in illumination. Algorithms describing different continuity criteria must be employed in order to obtain a reliable edge detection in an image. Moreover, as an straight line means a special case of an edge, detected edges have to be fit to straight lines. Fitting edges to straight segments can be accomplished by applying linear regression for the points comprising an edge in the image. Finally, the method has to find the endpoints of straight line segments, accounting for fragmentation or occlusions.
A set of pictures of the same scene may feature different kinds of viewpoint changes among captures, including camera rotations, zooms and translations. These changes in the camera viewpoint produce a morphological transformation of the primitives in the captured frame, which translates into displacements of the detected primitives, changes on their shape, distortions, fragmentation or even the impossibility to detect the same primitive in another image by employing the same operations that served to detect it in one of the pictures. Some of these transformations are not applicable to points, for instance a fragmentation: A point is either fully present or not, but it should not be such a thing as a detected fragmented point. Therefore, there are more morphologic transformations that can affect 2D line segments than the ones that can affect points, due to camera viewpoint change. Generally, prominent viewpoint transformations increase the difficulty in matching primitives, because the greater the transformation of the same primitives among different images of the scene, the greater the difficulty to match them.
Matching primitives between images is not always accurate, specially when dealing with line segments. When finding counterparts for primitives detected in other images, it is common to come out with several mismatched primitives. These wrongly matched primitives are referred to as matching outliers [11]. Matching outliers can produce that the description of the structure of groups of primitives can not be correctly compared to others, and employing inaccurate structure descriptions to propagate the matching to other images may cause problems when computing the final 3D abstraction. Some of the sources of the difficulties matching lines are because line segments are subject to more morphological transformations than points. The description of individual lines are therefore more subject to these transformations, and less truthfully at the end. This fact forces line matching methods to rely more on structure of neighborhoods than points. The accuracy of the description of these neighborhoods compared with the real morphological transformation of the lines it comprises are highly dependent on the ratio of matching outliers.
In the frame of 3D reconstruction from relations between feature points, known the relative position of two cameras and the position of one point on the first image, there is a constraint that forces the counterpart of this point on the second image to lay on a line. It is called epipolar constraint. But a single infinite 2D line represented in two images does not feature epipolar constraint. The only point-to-point valid correspondences in matched segments under a viewpoint change are their endpoints. For this case of a line segment, in order to estimate its position in 3D, is required to detect in the images both endpoints of the line segment. In some cases it may be difficult to accurately detect the end of a line segment in an image. For instance, a segment can end by merging with another edge under a different slope, progressively dimming until it vanishes, by intermittent occlusions, or being abruptly fragmented. Moreover, one or both segment endpoints may lay in the limits of the frame, and in this case it will not be possible to extract the 3D pose of the line.
The above mentioned tasks portrait the main differences between lines and points raised out during the engineering of a complete line-based 3D sketch generation method from images. For each stage of the method,specific tasks and problems have to be solved in the state-of-the art: detection of borders, matching lines over pairs of views, comparing the line matching performance against competition, relate the matched primitives among sets of more than two images, estimation of spatial lines, optimizing the abstraction and exploiting the resulting 3D structure.
2. Estimate 3D straight line segments
A 3D line can be thought as a multi-view entity that relates a perceivable line segment in the real world to its counterparts in images, given that these have been correctly detected and matched. The process of generating a 3D representation from different pictures of the scene is visually represented in Figure 1.
Figure 1.
Visual representation from [2]. It depicts the challenge of converting a set of 4 pictures into a 3D sketch featuring the line segments and camera axis. The 4 cameras are represented as three axis reference frame in red.
For the SfM problem, the poses of the cameras that took the pictures are not provided, and it is up to the SfM algorithm to simultaneously estimate the poses for the cameras and primitives. In the present case, SfM has to estimate the pose of the lines in space, relative to the cameras. The first requirement for the method is the calibration matrix K for each camera, which provides the transformation between each point in one image, in homogeneous coordinates, to a ray in Euclidean three-dimensional space. Secondly, SfM has to estimate the projection matrices P for the cameras, representing a map from 3D to 2D:
x=PX,E1
where x is a 2D point on the image, and X its projection in 3D space. K is intrisic to each camera, while P is extrinsic and embeds the 3D translation and rotation of the camera’s image plane. The estimated translation is valid up to scale.
A common space can be built to host the cameras and spatial lines. For this new common space the camera that took the first processed picture takes the place of the origin, and for the rest of cameras P can be estimated from the lines matched between the captured images. Alternatively, camera poses can also be retrieved from a feature-point based SfM pipeline and these cameras be employed for the estimation of spatial lines. For instance, the feature-point descriptor SIFT [5] can be used to match points in images with a low ratio of outliers. These feature point relations are obtained both in the foreground and background. A set of relations between points or lines in two images allows to estimate the homography constraints between both views by applying the 5-point algorithm [12] using the points or the segment endpoints. A purge of outliers can be performed employing RANSAC [13] for robust estimation. Therefore, a set of stereo 3D projections is obtained combining the available images pairwisely, and each stereo system featuring both camera poses and a point cloud. The objective is to obtain an unique 3D point cloud sketch, embedding all cameras and point matches. Hence, camera poses are sequentially stacked, relative to each other, in the new spatial reference frame. And the 3D estimations for the feature points in the new 3D space can be computed as the center of gravity for their position relative to the common camera in both stereo systems. Finally a sparse bundle adjustment [14] is used to minimize the pixel distance of the back-projected 3D point and the original observation of this point on each image in homogeneous coordinates. These reprojection errors on the planes of the cameras are minimized employing the Levenberg-Marquardt algorithm. The resulting keypoint-based 3D reconstruction contains the optimized 3D estimations for the cameras and the point cloud.
Several straight segment matching methods are based on texture descriptors [15, 16], coloring [17] or in keypoint-line projective invariants [18, 19]. Under these conditions, matching results will be influenced by the level of texture in the images. In the case that a low number of detected segments can be distinguished by employing image texture based descriptor, or in case that a low number of feature points are identified throughout the set of images, the resulting set of matched lines will not be satisfactory. On the other hand, if line matching is rooted on weak epipolar constraints [1], line matching will be highly dependent on the accuracy of the camera poses.
Extrinsic parameters for cameras are needed to project the matched lines into space. Having the same segment completely detected and without fragmentation for both views under viewpoint change, endpoints are the only points in a segment with known exact counterpart in the other image. Unfortunately, segment detection is not accurate in the location of the endpoints. Therefore, the most accurate abstractions will be the ones built rooted on camera extrinsics obtained from a dense feature point based SfM. As written above, known the projection matrices P of two cameras, a point on an image projects as a 3D ray in Euclidean space. And this 3D ray projects like an infinite 2D line on any plane different than the one that contains the point. Therefore, each 3D point Xp will have its image into an epipolar line ep contained in the image. As the unknown point is constrained into a line in the other image plane, analogously a segment will be constrained between both epipolar lines corresponding to the segment endpoints. This weak epipolar constraint can be employed for matching segments between images [1].
3. Geometric relations
A 3D abstraction method estimates the position of 3D line segments Γ = {Γ1, Γ2, Γ3, …, ΓN}, from an unordered sequence of images, taking from cameras with planes ϒ = {ϒ1,ϒ2,ϒ3,…,ϒM}. Straight lines are detected in the original images, put in correspondence among them, forward projected into space, and rewritten in homogeneous coordinates.
The 3D line based sketch {ϒ,Γ} is built from the knowledge of correspondences among line projections l on camera planes, and the intrinsics of all the cameras. The following paragraphs explain the linear triangulation of these observations, as performed from scale-space images. This allows to discriminate and weight down lines that have been detected on two or more scales with a different slope. The practical consequence is that prior to any 3D extrapolation of the observed lines, matching inliers with inconsistent endpoint location among scales on both images can be avoided, as these lines might introduce uncertainty in the estimation for the pose of the camera.
The camera poses P are estimated from the endpoint correspondences of l. The Essential matrix E is computed from the camera pairs, by using the Five-Point Algorithm [12], and RANSAC [13] for hypotheses generation. Having E and l, the relative camera rotation and translation among the first pair of cameras Pj=Rt are estimated using cheirality check and discarding the triangulated endpoints that are not in front of the cameras. The left camera is chosen to have the pose P1=I0, and the newly added cameras are stacked from this position in the unique reference frame.
The forward projection of lines in 3-space is described in the page 196 of Hartley and Zisserman’s book [20]. The 3D forward projection Γi of a line, bundled in the same reference frame, can be obtained using the DLT method on the set of stereo 3D camera back-projections. This is performed in homogeneous coordinates because it allows to consider line endpoints in the infinite. Therefore, from now on, when a 2D point is mentioned it will be supposed homogeneous coordinates. There exists a 3 × 3 matrix E, known as the essential matrix, such that if u and u′ are a pair of matched points, then u′Eu=0. If a sufficient number of matched points are known, the matrix E may be computed as the solution of an overdetermined set of linear equations. For the present problem, the internal calibration of the cameras is known, therefore it is possible to determine from E the relative placement of the cameras and hence the relative locations of the 3D points corresponding to the matched points. A linear triangulation method is projective-invariant because only camera and line distances are minimized.
The above described DLT method for lines starts with the segments on the pair of cameras ϒaϒb with the highest inlier ratio. Based on this first triangulation, the other cameras are appended to the 3D abstraction: The next camera ϒc is chosen according to the higher inlier ratio of line matching with ϒa and ϒb. Analogously, the following camera ϒn is picked among the ones with the higher inlier ratio of line matching with previously selected cameras. The detection of 2D lines l in the original images carry an uncertainty for the position of these observations. This uncertainty implies that no 3D point X will satisfy that their projections on cameras ϒ1 and ϒ2 are x1=P1X, x2=P2X respectively. Moreover, the image points do not satisfy the epipolar constraint x2Fx1=0. Therefore, a method that only minimizes the distances on the image from the estimations to the observations is required: A projective-invariant triangulation method. A linear triangulation [20] method does not depend on the projective frame in which X is defined.
The forward projection from a normalized 2D line observed on the camera image plane m, denoted by lim, is the plane PmTlim, so the condition for a point Xa to be in this plane is:
limTPmXa=0.E2
Each point Xa returns a linear equation in the entries of Pm. Denoting by xm,Ei and xm,Fi the forward projection of the endpoints of lmi, named XEi and XFi, under Pm, then any other 3D point on the line Xiμ=XEi+μXFi projects to a point:
ximμ=PmXi,E+μXi,F=xi,Em+μxi,Fm,E3
which is on the line segment lim.
In the described method, an unique reference frame is built. The world reference system is fixed onto the first camera, hence its camera matrix, PE, is computed with RE=I and TE=0. The extrinsics for the partner camera Pm on the baseline is obtained from the essential matrix by using RANSAC. Before the subsequent DLT triangulations with a new camera, its extrinsics are estimated also by RANSAC from the 2D-3D results of the already computed DLT. From here, new cameras will be added incrementally, just one per DLT iteration, in order to avoid DLTs between two uninitialized camera projection matrices.
For DLT it is required a set of observed line correspondences, ljm to ljn, matched among images. The projection on the image plane of camera m of an endpoint Xi,E of the spatial line Γj is denoted as xj,Em=PmXj,E. This point on the m-th camera plane is matched to its counterpart on the n-th camera xj,En=PnXj,E. Both equations can be combined into AXj,E=0, where A is the matrix of equation coefficients. It is built from the matrix rows Ar contributed from each correspondence, whose resemble the movement of each line between both views. Xj,E contains the unknowns for the endpoint position.
By using the cross product on the m-th camera: ljm×PmXj,E=0,
xmpm3TXj,E−pm1TXj,E=0,E4
ympm3TXj,E−pm2TXj,E=0,E5
xmpm2TXj,E−ymp1TXj,E=0E6
where xmym and xnyn are the coordinates of xj,Em and xj,En respectively. pmrT is the r-th row of Pm. It can be decomposed similarly for Pn, and compose the equation of the form AXj,E=0. Solving:
A=xmpm3T−pm1Tympm3T−pm2Txnpn3T−pn1Tynpn3T−pn2T.E7
The solution for the 4 equations of the over-determined problem (four equations for four homogeneous variables) is only valid up to scale. The set of points in space mapping to a 3D line Γj via Pm, is the plane PmΓj.
The result of the linear triangulation process is Γi and uj, represented in cartesian coordinates.
Every 3D segment Γi is estimated as the center of gravity of the estimations for the same line for each par of images. The set of line projections observed in ϒ is represented as l = {l11, l21, …, lN1, …, lNM}. A Line Feature is defined as a subgroup of projections from l of the same 3D line Γi. The Line Features are noted as L = {L1, L2, …, LN}. The 3D lines Γ are obtained by forward projecting the endpoints of l from pairs of camera planes of ϒ, by using linear triangulation, analogously to Direct Linear Transformation (DLT) [20]. The cameras ϒ are sequentially bundled in the same reference frame. The new ones are stacked according to the L-to-Γ correspondences, computed in the previous stereo pair of cameras. The merged estimations for 3D lines {Γi} are computed as the center of gravity of the spatial lines.
The 3D sketch {ϒ,Γ} generated by linear triangulation is used as input for an optimization algorithm. The least-squares optimization named Sparse Bundle Adjustment (SBA) [14] is based on the Levenberg–Marquardt algorithm, and uses as input the estimated camera extrinsics ϒ and the set Γ, now containing unique estimations for each 3D line [21].
The 3D estimations for lines and cameras are drawn in the same spatial sketch, altogether with the cameras. Next, these spatial line segments Γ are fit to different different planes P. Γ is therefore segmented into different groups according to the planes P, and so is done with their projections L. The group of Line Features fitted to the plane Pt is noted as Ft. The intersections of the coplanar lines Ft on the camera plane ϒj are the spatial points Ttj. Therefore, the algorithm can go back to the original images, now known which line segments are coplanar. The intersections of these coplanar lines on the images are described similarly as a feature point. Following this analogy, the descriptor for this feature point will be the pair of two coplanar lines drawing it. We have the correspondences of the straight lines accross images, so we can extrapolate these correspondences to their intersection for the cases where they are coplanar. Secondly, known the correspondences between these intersections, they can be triangulated analogously as it was performed in the first routine with the endpoints of l. The correspondences in Ttj are then fed into the linear triangulation algorithm, in order to create initial estimates for the 3D intersections by forward projecting Ttj. The set of estimations for the 3D points resembling the intersections is a sparse cloud, and it is denoted as R. Finally, and same as with the endpoints, the 3D intersections R enter the least-squares optimization. The SBA returns the new optimized estimations for ϒ, and the optimal 3D intersections R. The spatial line and camera pose estimations are corrected by forward projecting them from the newly estimated camera planes ϒ. This returns the final sketch {ϒ,Γ}. The high level diagram on Figure 2 shows the process described in this section.
Figure 2.
Figure from [2]. Graphic representation of the 3D abstraction layer of the method. The different cameras are represented as drones.
3.1 Bundle adjustment for line segments
In the case of feature points, the final position of the projected features relative to the camera poses is estimated throughout an optimization process. As a part of most SfM pipelines, bundle adjustment [14] is based on Levenberg-Marquardt, and it rearranges the poses of the cameras and 3D points. The cost function of this optimization process is engineered to find the minimum distance error between the reprojection of every 3D point onto each camera plane and their original observation. A limit value for the residual is usually set to stop the iterative process for the event of convergence, while another threshold is set to end the optimization when reaching a maximum number of iterations.
Along matched segments under a viewpoint change, the only point-to-point valid correspondences are their endpoints. Segment’s endpoint location are noticeably less accurate than a rotation and scale invariant feature point. Employing line endpoints as the sole set of geometrical constraints in the adjustment might not be adequate to improve the 3D sketch. Some of the reasons for this are that recurrent segment mismatches, fragmentation or the inaccurate placement of counterparts may prevent the convergence of the optimization. It is possible to perform a line-based Bundle Adjustment by converting the primitives into Plücker coordinates [20, 21] within the cost function of the optimisation process. This allows a reduction in the number of parameters and the computational cost.
3.2 How to compare the results with Ground Truth meshes
In order to prove the validity of a 3D abstraction method, it has to be benchmarked against a Ground Truth dataset for SfM, which includes both intrinsic and extrinsic parameters for the cameras. These are built with synthetic images from 3D models [22], or with real pictures [23] teamed with 3D model data including the pose of the cameras and the measurements from 3D scanning or Lidar. Both synthetic and real Ground-Truth datasets include a 3D model. The resulting point cloud is aligned with the Ground Truth mesh. The normal distance between the surface of the mesh and the points is computed. In order to assess how the generated sketch fits the Ground Truth model, the Mean Square Error of the distance between both spatial shapes is computed, because it acts as the natural loss function of a Gaussian distribution. In the case of 3D line sketch, in order to compare the sketch with the Ground truth mesh, the 3D straight segments must be discretized into points. To measure the difference in proportions between the generated 3D sketch and the Ground Truth mesh, the normal distance between the surface of the mesh and the discretized points on the lines is computed. Using the obtained error in the distances, discretized points on the lines are coloured to account how far they are from the surface of the mesh. There are several variables that condition the resulting 3D sketch number of images: Firstly, the number of images showing common elements of the scene is one of them. Secondly, the number of segments that can be matched between images. Thirdly, the transformation between both images might condition the matching inlier ratio, and hence, the number of segments correctly projected into space.
For 3D line sketching methods, the length of the final 3D lines will depend on the fragmentation of the detected lines, and its number is closely related to the number of line correspondences between the images. Therefore, results of 3D reconstructions will unavoidably depend on the performance of the method for stages before the spatial projection. Quantitative measurements for 3D abstraction are performed on Ground Truth datasets. The proportions of the generated sketch is measured based on the distance between the segments and the Ground Truth mesh.
Employing a feature-point based abstraction method is profitable for datasets with a sufficient number of pictures featuring textured surfaces, so a dense 3D point cloud can be created. For these 3D abstractions, cameras are located accurately due to the precision of the point rotation and translation invariants. This is the case of the results obtained by abstraction methods working altogether with SIFT pipelines [1, 22], but requiring dozens of high definition pictures with textured surfaces for SIFT to be able to accurately estimate the camera extrinsics.
There are real world applications of Computer Vision that does not always permit to obtain high definition pictures, in textured environments, without blurring and digital noise. For these applications it can be advantageous to estimate the camera extrinsics independently of any feature point 3D reconstruction [2]. Figure 3 shows a quantitative comparison of the methods [2] and [1] with just 6 and 8 images chosen from the dataset. Figure 4 increases the number of images to 10 and 12. The test cases are labeled as S6, comprising image numbers {6,9,86,46,49,126} from [22], S8 further add two more images {89,129} to the list, S10 includes {8,10,12,88,90,48,50,52,128,130}, and S12 further adds images {92,132} to the latter. The resulting 3D line sketches from both sides of the house are aligned by using common lines. This completed sketch is finally aligned to the Ground Truth in order to measure the precision. Note that this experiment takes into account just a the variation of the number of images in the dataset [22]. The results show that the method [2] obtains more usable results for a low number of images, and the results of method [1] are only more adequate than method [2] when the number of images gets close to a dozen. The spatial lines are colored attending to its distance to the surface of the Ground Truth mesh.
Figure 3.
Figure from [2]. Quantitative comparison using the sets S6 and S8. This figure is better viewed on a screen with a 4x zoom. (a) Sample of the set. (b) and (c) [2] against S6, resulting in 175 lines. (d) and (e) Same superposed onto the Ground Truth mesh. (f) Histogram of distances to Ground Truth with [1] method. The maximum distance to be accounted is set to be 0.8, already considered as outlier. (g) Sparse atomic lines returned by [1] method. (h) to (l) [1] against the set S8, with 294 segments. (m) and (n) same measurements for the result by [1]. (o) shows the histogram for this latter result.
Figure 4.
Figure from [2]. Quantitative comparison using the sets S10 and S12. This figure is better viewed on a screen with a 4x zoom. (a), (b) and (c) [2] against S10. The obtained 475 lines have been discretized in points. The distance from each point in the cloud to the surface of the Ground Truth mesh is represented in colors. (d) and (e) Same superposed onto the Ground Truth mesh. (f) Histogram of distances to Ground Truth with the [2] method. The maximum distance to be accounted is set to be 0.8, already considered as outlier. (g) Sparse atomic lines returned by the method [1]. It has been aligned with the Ground Truth mesh. (h) to (l) Same for the method [2] against the set S12, with 556 segments. (m) and (n) same measurements for the result by [1]. (o) shows the histogram for this latter result.
4. Conclusions
A 3D abstraction method receives as input the camera intrinsic parameters and several pictures of the scene. There are two different approaches: The first one does not require the camera extrinsics estimated from an external SfM pipeline, nor the Ground Truth camera poses [2]. It sources the line correspondences from a line matching method, and is able to generate 3D sketches from sets of pictures. This kind of approaches get an edge against datasets with low number of images, or when these present corrupted texture, blurring, and low definition images where the feature point descriptor fails to detect a fair number of keypoints. The reduced number of correspondences limit the thickness of the point cloud generated by the SfM pipelines, and therefore the accuracy of the estimated camera extrinsics. With inaccurate estimations for the cameras, exploiting homography constraints is not adequate to source line correspondences. Oppositely, [2] is able to reconstruct simple line-based sketches with fair precision and number of lines. It required lower number of images to obtain more complete abstractions than method [1]. The range of scenarios where it is advantageous to use method [1] for 3D abstraction includes sets of pictures of simple objects, with low texture, poor illumination, low resolution, blurring or under other conditions that make difficult the success of a point based algorithm. In these scenarios it outperforms the competition in terms of quantity of lines, precision and completeness of the abstraction. Another conclusion is that camera extrinsics are unavoidably required for 3D abstractions featuring many lines, because the estimation for the camera poses will not be accurate if the line matching method returns matching outliers or line fragmentation.
On the other hand, for datasets with moderate number of images, which clear textures, the second approach can be profitable. In this case, the geometric relations from the related points among the images will permit the feature point based pipeline to generate a moderately dense 3D point cloud. In this case, the poses of the cameras obtained by the point based pipeline can be trusted, and used as basis for line matching and linear projection to generate the 3D sketch. The results obtained with method [1] with datasets of hundreds of images are very good. An abstraction using this method will team perfectly with a dense reconstruction.
Both approaches are valid for their range of applications. The first one is valid for difficult datasets with noise and low number of images. The second approach will shine with datasets with high texture and many pictures, because it will will profit of the high precision obtained from feature point based 3D reconstruction pipelines for locating the cameras.
Acknowledgments
The original research work [2] received financial support from the Xunta de Galicia through grant ED431C 2017/69 and Xunta the Galicia (Centro singular de investigación de Galicia accreditation 2016-2019) and the European Union (European Re gional Development Fund - ERDF) through grant ED431G/08.
Conflict of interest
The author declares no conflict of interest.
\n',keywords:"structure from motion, 3D abstraction, SLAM, 3D sketch, 3d reconstruction",chapterPDFUrl:"https://cdn.intechopen.com/pdfs/75321.pdf",chapterXML:"https://mts.intechopen.com/source/xml/75321.xml",downloadPdfUrl:"/chapter/pdf-download/75321",previewPdfUrl:"/chapter/pdf-preview/75321",totalDownloads:154,totalViews:0,totalCrossrefCites:0,totalDimensionsCites:0,totalAltmetricsMentions:0,impactScore:0,impactScorePercentile:47,impactScoreQuartile:2,hasAltmetrics:0,dateSubmitted:"May 12th 2020",dateReviewed:"January 21st 2021",datePrePublished:null,datePublished:"July 7th 2021",dateFinished:"February 18th 2021",readingETA:"0",abstract:"This chapter serves as an introduction to 3D representations of scenes or Structure From Motion (SfM) from straight line segments. Lines are frequently found in captures of man-made environments, and in nature are mixed with more organic shapes. The inclusion of straight lines in 3D representations provide structural information about the captured shapes and their limits, such as the intersection of planar structures. Line based SfM methods are not frequent in the literature due to the difficulty of detecting them reliably, their morphological changes under changes of perspective and the challenges inherent to finding correspondences of segments in images between the different views. Additionally, compared to points, lines add the dimensionalities carried by the line directions and lengths, which prevents the epipolar constraint to be valid along a straight line segment between two different views. This chapter introduces the geometrical relations which have to be exploited for SfM sketch or abstraction based on line segments, the optimization methods for its optimization, and how to compare the experimental results with Ground-Truth measurements.",reviewType:"peer-reviewed",bibtexUrl:"/chapter/bibtex/75321",risUrl:"/chapter/ris/75321",book:{id:"8734",slug:"applications-of-pattern-recognition"},signatures:"Roi Santos Mateos, Xose M. Pardo and Xose R. Fdez-Vidal",authors:[{id:"24139",title:"Dr.",name:"Xose Ramón",middleName:null,surname:"Fdez-Vidal",fullName:"Xose Ramón Fdez-Vidal",slug:"xose-ramon-fdez-vidal",email:"xose.vidal@usc.es",position:null,profilePictureURL:"//cdnintech.com/web/frontend/www/assets/author.svg",institution:null},{id:"24140",title:"Prof.",name:"Xose M.",middleName:null,surname:"Pardo",fullName:"Xose M. 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Conclusions",level:"1"},{id:"sec_8",title:"Acknowledgments",level:"1"},{id:"sec_11",title:"Conflict of interest",level:"1"}],chapterReferences:[{id:"B1",body:'Manuel Hofer, Michael Maurer, and Horst Bischof. Improving sparse 3d models for man-made environments using line-based 3d reconstruction. In 3D Vision (3DV), 2014 2nd International Conference on, volume 1, pages 535–542. IEEE, 2014'},{id:"B2",body:'Santos, Roi, Xose M. Pardo, and Xose R. Fdez-Vidal. “Scene wireframes sketching for Unmanned Aerial Vehicles.” Pattern Recognition 86 (2019): 354-367'},{id:"B3",body:'Zhou, Hang, et al. “Uncertainty Analysis of 3D Line Reconstruction in a New Minimal Spatial Line Representation.” Applied Sciences 10.3 (2020): 1096'},{id:"B4",body:'Nieto, Marcos, and Luis Salgado. “Real-time robust estimation of vanishing points through nonlinear optimization.” Real-Time Image and Video Processing 2010. Vol. 7724. International Society for Optics and Photonics, 2010'},{id:"B5",body:'Lowe, David G. “Object recognition from local scale-invariant features.” Proceedings of the seventh IEEE international conference on computer vision. Vol. 2. Ieee, 1999'},{id:"B6",body:'Alcantarilla, Pablo Fernández, Adrien Bartoli, and Andrew J. Davison. “KAZE features.” European Conference on Computer Vision. Springer, Berlin, Heidelberg, 2012'},{id:"B7",body:'Micusik, Branislav, and Jana Kosecka. “Piecewise planar city 3D modeling from street view panoramic sequences.” 2009 IEEE Conference on Computer Vision and Pattern Recognition. 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IEEE, 2010'},{id:"B23",body:'Strecha, Christoph, et al. “On benchmarking camera calibration and multi-view stereo for high resolution imagery.” 2008 IEEE Conference on Computer Vision and Pattern Recognition. Ieee, 2008'}],footnotes:[],contributors:[{corresp:"yes",contributorFullName:"Roi Santos Mateos",address:"roi.santos@usc.es",affiliation:'
University of Santiago de Compostela, Spain
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1. Introduction
In terms of comfort and exuberant use, cotton fibre is considered the most classical fibre in garment technology. Versatility of cotton fibres ranging from very finer to very courser and structure of cotton yarns such as single to ply are considered as decisive factors of selection regarding their use in apparel production. On the other hand, the comfort property, being one of the prime features of woven fabric used as a garment, is greatly influenced by the structure of constituent yarns in that particular fabric. Comfort evaluation includes mainly vapour and liquid transmission properties of yarn and fabric at constant atmospheric conditions and constraints. Liquid transmission includes water absorbency and wicking [1, 2].
Absorbency is used to describe the ability of a fabric to take in moisture—an important feature that influences a variety of other factors such as skin comfort, static build-up, shrinkage, water repellency and wrinkle recovery. One of the most common occurrences in the manufacturing and usage of textile materials is liquid flow. Wicking is the spontaneous transfer of a liquid into a porous structure caused by capillary forces. Therefore, study of capillary flow in textile media is very important. When the free energy of the solid-gas interface surpasses that of the solid-liquid interface, capillary phenomena occur. A liquid that does not wet fibres cannot wick into a fabric, and wicking can only take place when fibres are assembled with capillary spaces. But the objective of this is to present an overview only in wicking property of textiles.
Study of wicking in textile material is of great interest for two main reasons. Firstly, it allows a better understanding of liquid-fibre contact in order to characterise any liquid flow of spin finishes, dyeing or coating of either fabrics or yarns. Secondly, it enables the characterisation of textile structures, their porosity resulting from the capillaries formed by the inter-filament spaces in which the liquid flows [3]. Moisture absorption is intimately linked to the comfort of garments made from cellulosic fibres. The term wetting is usually used to describe the displacement of solid-air interface with solid liquid interface. Wetting behaviour is commonly characterised by the value of the contact angle within the liquid [4]. The wetting and wicking behaviour of the fibrous structure is a critical aspect of performance of products such as sports clothes, hygiene disposable materials and medical products. Clothing comfort is influenced by the wetting and wicking processes that occur during wear.
Therefore, a thorough understanding of liquid transmission behaviour inside various intermediate forms of textiles is obviously needed through absorbency and wicking phenomena of yarns and fabrics. As the yarns are composed of fibres with a structured arrangement, any change of this arrangement by twisting and plying creates different sort of wicking behaviour on them and in turn, the fabrics made out of these yarns along with its varying weave forms and directions must exhibit different nature of wicking effects. The findings that are interlinking between fabric wicking and corresponding yarn wicking are always a matter of interest to study the nature of absorbency specially for textiles made out of natural fibres and hence, are elaborated progressively in this chapter.
2. Lucas-Washburn theory
The so-called wicking (or absorbency) rate is of great importance for both scientific and practical uses. The Lucas-Washburn idea provides a more scientific definition of the wicking rate. This theory deals with the rate of a liquid drawn into a circular tube via capillary action. A capillary like this is a severely simplified representation of a pore in a true fibrous media with a complex structure. For laminar viscous flows, theory is a specific form of the Hagen-Poiseuille law state Landau and Lifshitz. According to this law, the volume dV of a Newtonian liquid with viscosity μ that wets through a tube of radius r and length h during dt is given by the relation:
dV/dt=πr4p1–p2/8hμE1
where p1 – p2 is the pressure difference between the tube ends. The capillary force and gravitation both contribute to the pressure difference here. The angle between the tube axis and the vertical direction is denoted by β, while the contact angle of the liquid against the tube wall is denoted by θ. The value of the capillary pressure p1 is:
p1=2γcosθ/rE2
While hydrostatic pressure p2 is:
p2=hζgcosβ,E3
where γ denotes the liquid surface tension, ζ is liquid density, g is the gravitational acceleration, and h, in this case, is the distance travelled by the liquid measured from the reservoir along the tube axis. This distance obviously is the function of time, h = h (t), for a given system. The Lucas-Washburn equation is obtained by substituting the values p1, p2 and h(t) into Eq. (1), expressing the liquid volume in the capillary V as πr2h:
dV/dt=rγcosθ/4μh–r2ζgcosβ/8μE4
For a given system, parameters such as r, γ, θ, ζ, g and β remain constant. We can then reduce the Lucas-Washburn equation (4) by introducing two constants,
K′=rγcosθ/4μandL′=rζgcosβ/8μE5
into a simplified version,
dh/dt=K′/h–L′E6
The above relation is a non-linear ordinary differential equation that is solvable only after ignoring the parameter L′; this has a physical interpretation when either the liquid penetration is horizontal (β = 900 C) or r is small or the rising liquid height h is low that K′/h > > L′ or L′ → 0, and the effects of the gravitational field are negligible and the acceleration g vanishes. The Lucas-Washburn equation (6) could thus be solved with ease:
h=√2K′t.E7
The result satisfies the initial condition h = 0 for t = 0.
Despite the intricate, noncircular, non-uniform and nonparallel nature of the pore spaces, the Lucas-Washburn technique provides an approximation tool for investigating the wicking and wetting behaviour of textiles. In the field of liquid sorption in a porous area, Washburn (1921) has expressed the following equation:
H=Ct0.5E8
where H is the wicking height (m); C, the capillary liquid transport constant. The capillary force causes liquid to flow through a capillary channel, as shown in the equation above. The radius of the capillary channel, the contact angle between the liquid and the capillary channel and the rheological qualities of the liquid all influence the capillary force [5].
3. Wetting
The displacement of a solid-air interface with a solid-liquid contact is commonly referred to as ‘wetting’. Two separate equilibrium regimes may be identified when a small liquid droplet comes into contact with a flat solid surface. Complete wetting with a zero-contact angle or partial wetness with a finite contact angle is shown in Figure 1. The equilibrium at a solid-liquid boundary is commonly described by the Young’s equation:
Figure 1.
A small liquid droplet in equilibrium over a horizontal surface: (a) partial wetting, mostly non-wetting; (b) partial wetting, mostly wetting; (c) complete wetting.
γSV–γSL–γLVcosθ=0E9
where, γSV, γSL and γLV denote interfacial tensions between solid/vapour, solid/liquid and liquid/vapour, respectively, and θ is the equilibrium contact angle.
The parameter that distinguishes partial wetting and complete wetting is the so-called spreading parameter S, which measures the difference between the surface energy (per unit area) of the substrate when dry and wet:
S=Esubstratedry–EsubstratewetE10
Or,
S=γSV–γSL+γLVE11
The liquid spreads entirely to lower its surface energy (θ = 0) if the parameter S is positive. The end result is a layer with a nano-scopic thickness that results from molecular and capillary forces competing. If S is negative, the drop does not spread out and instead forms an equilibrium spherical cap resting on the substrate with a contact angle of. When θ ≤ π/2, a liquid is said to be ‘mainly wetting’, while when θ > π/2, it is said to be ‘primarily non-wetting’. When a surface is connected with water, it is referred to as ‘hydrophilic’ when it is θ ≤ π/2 and ‘hydrophobic’ when it is θ > π/2 [6].
3.1 Wicking
Wicking is the capillary-driven spontaneous flow of a liquid in a porous medium. Wetting causes capillary forces; hence, wicking is the result of spontaneous wetting in a capillary system. A meniscus is created in the simplest case of wicking in a single capillary tube as shown in Figure 2. A pressure difference across the curved liquid/vapour contact is caused by the surface tension of the liquid. The value for the pressure difference of a spherical surface was deduced in 1805 independently by Thomas Young and Pierre Simon de Laplace and is represented with the so-called Young-Laplace equation [6]:
Figure 2.
Wicking in a capillary.
∆P=γLV1R1−1R2E12
For a capillary with a circular cross section, the radii of the curved interface R1 and.
R2 are equal. Thus:
∆P=2γLV/RE13
where,
R=r/cosӨE14
and r is the capillary radius. Since the capillary spaces in a fibrous assembly are not uniform, the effective capillary radius re is utilised instead, which is usually an indirectly determined parameter.
3.2 Capillary theory
Capillary action is governed by the properties of the liquid, the fibre surface wetting characteristics and the geometric configurations of the porous medium. In a capillary, liquid rises due to the net positive force (ΔP) across the liquid-solid interface.
ΔP=P–δgh,E15
where δ = liquid density in g/cc, g = gravitational acceleration of 980.7 cm/s2, height of liquid rise in cm = h, the capillary pressure (p) is described by the initial wetting force (Fwi) in the capillary area (πri2):
P=Fwi/πri2=2πriγcosθ/πri2=2γcosθE16
where, γ = liquid surface tension in dyne/cm.
ri = radius inside the capillary in cm and.
θ = liquid-solid contact angle.
Where capillary pressure (P) is greater than the weight of the liquid (δgh), the positive forces drive the liquid upward. Upon reaching equilibrium where P – δgh, the net driving force ΔP becomes zero. The liquid stops rising at the equilibrium height (h).
4. Liquid transport system
Water transport in yarns is only slightly influenced by the wetting properties of the individual fibre materials and depends mainly on the wetting behaviour of the whole yarn. The rate of water transport decreases as the roughness of the yarn increases due to the random arrangement of its fibres [7]. This is thought to be dependent on two factors that are directly related to capillary water transfer. (a) As the yarn roughness increases, so does the effective advancing contact angle of water on the yarn. (b) As the fibre arrangement gets more random, the capillary continuity generated by the yarn fibres appears to decrease. Most elements of water transport behaviour are accounted for by the penetration of capillaries created by the fibres in the yarns. Both the amount of water carried by the fabric and the distance that it travels in unit time are influenced considerably by the randomness of the arrangement of fibres in the yarns [8].
Perwuelz et al., on the other hand, worked on liquid organisation during capillary rise in yarns. It was found that capillary rise was dependent on the capillary diffusion coefficient of the yarn, and twist increase reduced the average value of the diffusion coefficients [9]. Twist retraction can cause fibres around the yarn centre to buckle when a high twist is applied into the yarn. This can damage the pore structures between fibres and influence the wicking behaviour [10]. Moreover, another study showed that wicking velocity increased with the increase in cross-sectional area of yarn and decrease in liquid viscosity [11]. In accordance with the literature, packing density of the yarns also influences wicking property. Compact yarns have higher packing density than conventional ring spun yarns, as a result of that they show lower wickability [12].
4.1 Wicking in yarn
Researcher investigated the wicking property of the yarns and found that the wicking behaviour of the yarns improved with the increase in the cross-sectional area due to a larger number of capillaries in yarns [13]. In the case of plied yarns, it is been found that the difference of wicking height of 2-ply and other higher plied yarns is more in finer yarn (40s) as compared with coarser yarn (20s) [14]. The difference of wicking height between 2-ply yarn and a higher number of yarns gradually decreases from finer yarn to coarser yarn [15].
4.1.1 Effect of yarn modification on water absorbency
It is evident that as the fibres become coarser, the water absorbency increases. The explanation for this could be due to coarser fibres’ higher bending rigidity [16, 17] and a decrease in the number of fibres in the yarn cross section. As a result, the bulkiness of the yarn increases [18, 19]. Increased water absorbency is also linked to the availability of more pore volume in yarn structures [19].
It has been noticed that when yarn coarseness increases, cloth water absorbency increases at first, then declines. The explanation for this could be due to a decrease in yarn structure compactness [20] and an increase in yarn bulkiness, which increases the availability of air spaces in the yarn structure, resulting in an increase in water absorbency [21, 22].
It has been discovered that when the sheath content of the yarn increases, fabric’s water absorbency also increases. The explanation for this could be due to an increase in fabric openness [23] and yarn bulkiness when the sheath is removed, resulting in more air gaps in the yarn structure, which leads to an increase in water absorbency [20].
4.1.2 Effect of yarn modification on wicking characteristics
It is evident that as the fibre gets coarser, the fabric wicks more. The explanation for this could be due to coarser fibres’ higher bending rigidity [18] and a decrease in the number of fibres in the yarn cross section. As a result, the bulkiness of the yarn increases [19, 23]. Increased wicking is caused by the availability of increased pore space within the yarn structure [24].
It has been noticed that when yarn coarseness increases, fabric wicking increases at first, then decreases. Because of the decrease in compactness of yarn structure [20] and rise in bulkiness of yarn, the size of the pores initially increases as the yarn becomes coarser, increasing the availability of air spaces in the yarn structure. Wicking increases as a result of this [25]. However, beyond a certain degree, the pore structure opens up, slowing the flow of water through the pores.
Fabric wicking is observed to increase when the proportion of sheath fibres rises. The explanation for this could be due to an increase in fabric openness [21] and yarn bulkiness when the sheath is removed, resulting in more air gaps in the yarn structure [23]. Furthermore, parallel fibre arrangement creates correct channelling within the yarn, resulting in increased wicking [26, 27].
4.2 Wicking in fabric
Fabric with a high and consistent absorbency is desirable in almost every wet finishing procedure and many finished fabrics. The wicking property of materials affects their absorbency. When a fabric is entirely or partially submerged in a liquid, or in touch with a small amount of liquid, such as a drop placed on the fabric, wicking occurs. As a result, capillary penetration of a liquid can occur from either an infinite (unlimited) or a finite (limited) reservoir. Immersion, transplanar wicking and longitudinal wicking are the wicking processes that occur from an infinite reservoir. A drop placed on the cloth surface demonstrates wicking from a restricted reservoir [28]. The places of interlacement between warps and wefts were constantly formed in horizontal and vertical directions as fluid flow split. The horizontal yarns (either warp or weft, depending on the test direction) served as fluid reservoirs to wick further along the vertical yarns [29].
4.2.1 Effect of fabric parameters on wicking and its application as technical textiles
Researchers have discovered that fabrics with equally distributed float wick slower and horizontally striped fabrics wick quicker. Because the floats of threads in horizontally striped fabrics are positioned on the edge of the horizontal stripes and spread throughout the entire fabric surface, this happens. This uneven structure could explain why horizontally striped materials have a higher wicking rate. The pace of warp and weft way wicking differs slightly, and in some situations, the rate of weft way wicking is larger than the rate of warp way wicking. This could be caused due to tension differences between warp and weft threads. The rate of wicking for uniformly dispersed floats increases as weave factor P1 increases, which is due to the increase in floats in the fabrics [30]. Fabrics made of ring yarn wick faster than fabrics made of compact yarn [31]. Moisture management behaviour of knitted fabric has been studied from structurally modified ring and vortex spun yarn where the air permeability, water vapour permeability and total absorbency of the knitted fabric made from changed yarn all improved significantly, whereas the wicking characteristic decreased [32]. Fabrics composed of coarser yarns (40s Ne) wick more quickly than fabrics made of finer yarns (50s Ne). Fabrics behave in the same way that yarns do when it comes to wicking. The difference in wickability between plain weave and twill weave fabrics grows as the constituent yarn fineness increases. This variation is substantially more noticeable in diagonal wicking than in warp- and weft-way wicking [33]. The Lucas-Washburn equation was found to be suitable for analysing the wicking behaviour of woven cotton fabrics, and the wicking height square had a positive and good correlation with time in both the warp and weft directions, according to Zhu et al. [34]. Wicking height decreases with increasing weft yarn density as it leads to a decrease in porosity due to increased warp yarn crimp [35].
Using a sink time technique, the wettability of various terry towel fabrics was tested, and it was discovered that fabrics with higher loop density (repeat with 3-pick) sink faster than those with lower pick density (4, 5 and 6-pick weaves). Vertical wicking studies reveal that materials with a 3-pick density wick the fastest, followed by fabrics with 4, 5 and 6-pick density [36]. Moisture management is used in applications such as active athletics, exercise garments, work clothing, intimate apparel and footwear to avoid or limit liquid collection on the wearer’s skin owing to perspiration. This is accomplished by rapidly wicking or diffusing the liquid through an inner hydrophobic fibre layer to an outside hydrophilic layer, then evaporating it into the atmosphere. Sportwool is a two-layer sportswear with good moisture management qualities that is utilised in a variety of sports apparel. The inner layer, which is closest to the skin, is made up of chemically treated ultrafine Merino wool fibres (˂20 μm). The exterior layer is completely constructed of polyester filament yarn. Wool fibres have a high-water vapour permeability, which allows heat and moisture to be transferred from the skin to the outside surface, where it can escape due to wind speed and body movement [37]. A multi-layer construction is appropriate for sportswear [38, 39]. According to D’Silva and Anand [38], in a two-layer construction, the wicking layer is made up of synthetic fibres, such as micro-denier polyester, while the absorbent and evaporating layer is commonly cotton or rayon.
Many healthcare and personal hygiene items require liquid flow management in terms of liquid volume and flow rate elements that are acceptable for the end use. The incorporation of effective capillary systems into the final product allows for controlled liquid flow. Hygiene goods are made up of different layers of materials with different properties that allow liquid or moisture to drain swiftly away from the inner surface of the material in contact with the wearer’s body. Wicking and wetting principles are applied to multilayer protective clothing. The outer layer of protective clothing consists of permeable fabric or a liner or a layer made of carbon-loaded foam. To reduce the wetting due to body fluid, the outer layer is treated with a fluoro-chemical, and this reduces the surface energy, and thereby, the wetting is reduced [40]. Geotextiles are permeable fabrics that can hold solid items in place while allowing water to pass through. Due to their low cost, consistent qualities and convenience of placement, they have been widely used as drainage, separation and filter materials in geotechnical and geo-environmental activities for about 30 years. The primary goal of geotextiles is to allow water to flow through the filter into the drain over the course of the project while keeping soil particles in place and avoiding migration through the filter [40]. Natural geotextiles are now being used such as jute geotextiles (JGT) where biodegradability of JGT is an advantage when control of surficial soil erosion is considered. It acts as mulch, attenuates extremes of temperature, adds micronutrients to the soil, leaves fibrous residues that improve hydraulic conductivity of soil and thus eases dissipation of pore water pressure [41].
5. Experimental
The study focused on 100% cotton fabrics and their constituent cotton yarns, which included plied yarn for the warp and single yarn for the weft. During the preparation of the yarns, three (3) different counts, namely 20s, 30s and 40s Ne, were prepared from 0.9 s Ne cotton roving using a TRYTEX Miniature Ring Spinning machine for specific TM values of 4 (in indirect cotton count system), ensuring that the helix angle of fibres remained constant in all yarn structures. For all of the yarns, machine parameters such as the ring frame machine’s spindle speed were set to 10,000 rpm.
Second, after necessary assembly winding and a portable laboratory winder, the yarns in the 20s, 30s and 40s were made 2-ply each using a TRYTEX Miniature TFO machine. Then, using 2-ply of each count as warp and single yarn of each count as weft, 1/1 plain and 2/1 twill weave fabric samples were produced, with their respective sample codes provided in Table 1.
Sample No.
Fabric construction
Sample code
Plain weave
Twill weave
1
2/20 as warp and 20s as weft
FP1
FT1
2
2/30 as warp and 30s as weft
FP2
FT2
3
2/40 as warp and 40s as weft
FP3
FT3
Table 1.
Fabric sample and used codes.
Thus, a total of six yarn samples and six fabric samples were prepared for this study. All the yarn (single and plied) and fabric (plain and twill) samples had undergone a scouring process with the standard recipe as wicking is highly correlated to wetting so it is a prerequisite that the sample should be as hydrophilic as much as possible. All the scoured samples (yarns and fabrics) were subsequently used for testing of wicking phenomena after conditioning the fabric in standard atmospheric conditions for 48 h. The basic parameters of fabrics are determined in Table 2.
Sample No.
Sample codes
Thread density
Cloth cover factor
Ends/inch
Picks/inch
1
FP1
53
60
22.17
2
FP2
58
60
20.07
3
FP3
62
60
18.64
4
FT1
54
63
22.57
5
FT2
58
63
20.33
6
FT3
59
63
18.46
Table 2.
Thread density and cloth cover factor of respective fabric samples.
After setting up the experimental set-up in the testing centre, all of the yarn and fabric samples were evaluated for wicking parameters. Different yarn and fabric samples are initially built up in accordance with DIN 53924. Fabric pieces of 200 mm × 25 mm were used in the experiment. A beaker was placed beneath the yarn and fabric strip such that the yarn and fabric strip’s end was dipped into the water. Figures 3 and 4 demonstrate how yarns and fabric samples were hung in a stand by a clip. The laboratory travelling microscope was placed at the water level, and readings of the water level were taken at regular intervals.
Figure 3.
Wicking set-up for yarn.
Figure 4.
Wicking set-up for fabric.
6. Wicking behaviour of woven fabrics and its interrelation with their constituent yarns
As reviewed, wicking behaviour has been evaluated classically in terms of wicking height of the respective fabrics and its constituent yarns. Wicking height of fabrics has been shown in three different directions, and ultimately, related results have been used to establish the relationship between fabric wicking and its constituent yarn wicking phenomena.
6.1 Effect on wicking height (with respect to time) in various directions (warp-way, weft-way and diagonal-way) of fabrics as well as their constituent yarns
Tables 3–5 indicate the values of wicking height as a function of time as recorded in the trials for different orientations of fabrics and their constituent yarns in the 20s, 30s and 40s, respectively. Figure 5 depicts the liquid flow for a specific set of warp and weft threads in the warp, weft and diagonal directions of fabric samples.
Time (min)
Wicking height of yarn (cm)
Wicking height of FP1 (cm)
Wicking height of FT1 (cm)
2ply
Single
Warp
Weft
Diagonal
Warp
Weft
Diagonal
0.5
3.2
2.2
0.3
0.3
0.2
0.5
0.2
0.3
1
4.4
3.0
0.6
0.4
0.4
1.0
0.5
0.6
2
5.9
3.7
1.4
0.9
0.7
1.7
1.1
1.3
3
6.9
4.5
2.0
1.4
1.0
2.3
1.5
1.6
4
7.6
5.2
2.6
2.1
1.4
2.6
2.0
1.9
5
8.1
5.7
3.0
2.4
1.8
3.0
2.4
2.5
10
10.2
7.3
3.5
2.7
2.3
3.6
2.7
2.9
20
12.3
8.1
4.1
3.0
2.5
4.0
2.9
3.1
30
13.7
8.2
4.4
3.2
2.7
4.2
3.1
3.3
60
13.7
8.2
4.9
3.4
3.0
4.5
3.2
3.4
120
13.7
8.2
4.9
3.4
3.1
4.5
3.2
3.4
Table 3.
Wicking height of fabric samples (with codes) in different directions along with its constituent 2/20s Ne plied yarns (used as warp) and 20s Ne single yarns (used as weft).
Time (min)
Wicking height of yarn (cm)
Wicking height of FP1 (cm)
Wicking height of FT1 (cm)
2ply
Single
Warp
Weft
Diagonal
Warp
Weft
Diagonal
0.5
3.2
2.2
0.3
0.3
0.2
0.5
0.2
0.3
1
4.4
3.0
0.6
0.4
0.4
1.0
0.5
0.6
2
5.9
3.7
1.4
0.9
0.7
1.7
1.1
1.3
3
6.9
4.5
2.0
1.4
1.0
2.3
1.5
1.6
4
7.6
5.2
2.6
2.1
1.4
2.6
2.0
1.9
5
8.1
5.7
3.0
2.4
1.8
3.0
2.4
2.5
10
10.2
7.3
3.5
2.7
2.3
3.6
2.7
2.9
20
12.3
8.1
4.1
3.0
2.5
4.0
2.9
3.1
30
13.7
8.2
4.4
3.2
2.7
4.2
3.1
3.3
60
13.7
8.2
4.9
3.4
3.0
4.5
3.2
3.4
120
13.7
8.2
4.9
3.4
3.1
4.5
3.2
3.4
Table 4.
Wicking height of fabric samples (with codes) in different directions along with its constituent 2/30s Ne plied yarns (used as warp) and 30s Ne single yarns (used as weft).
Time (min)
Wicking height of yarn (cm)
Wicking height of FP1 (cm)
Wicking height of FT1 (cm)
2ply
Single
Warp
Weft
Diagonal
Warp
Weft
Diagonal
0.5
3.2
2.2
0.3
0.3
0.2
0.5
0.2
0.3
1
4.4
3.0
0.6
0.4
0.4
1.0
0.5
0.6
2
5.9
3.7
1.4
0.9
0.7
1.7
1.1
1.3
3
6.9
4.5
2.0
1.4
1.0
2.3
1.5
1.6
4
7.6
5.2
2.6
2.1
1.4
2.6
2.0
1.9
5
8.1
5.7
3.0
2.4
1.8
3.0
2.4
2.5
10
10.2
7.3
3.5
2.7
2.3
3.6
2.7
2.9
20
12.3
8.1
4.1
3.0
2.5
4.0
2.9
3.1
30
13.7
8.2
4.4
3.2
2.7
4.2
3.1
3.3
60
13.7
8.2
4.9
3.4
3.0
4.5
3.2
3.4
120
13.7
8.2
4.9
3.4
3.1
4.5
3.2
3.4
Table 5.
Wicking height of fabric samples (with codes) in different directions along with its constituent 2/40s Ne plied yarns (used as warp) and 40s Ne single yarns (used as weft).
Figure 5.
Wicking phenomena in fabric for various directions such as (a) warp way, (b) weft way and (c) diagonal way.
The tabulated findings show a few generalised observations about the behaviour of yarn wicking in comparison to fabric wicking. First and foremost, it is well established that ply yarns usually provide superior wicking than single yarns of the same fineness due to the presence of densely populated fibres in the plied structure versus a single form of yarn. It is also discovered that the wicking height of constituent yarns, whether plied (used as a warp) or single (used as a weft), of any fineness (expressed by counts), is higher than that of their respective fabrics, regardless of the direction of testing for plain weave samples. This usual phenomenon can be understood specifically for plain weave due to the compact fibrous structure of yarns in comparison to the porous-interlaced structure of fabrics made out of this constituent yarn resulting in much better capillary action facilitating higher liquid transmission inside the structure. An exception to this trend has been observed for twill fabrics produced from medium and finer count yarns when viewed with respect to wicking of single yarn structure. Lesser number of interlacements may predominate for the attainment of higher wicking height in a twill weave in comparison to that of a single yarn.
However, a thorough explanation of the relative wicking phenomena is needed to set up a relationship between fabric wicking in various directions with respect to their constituent yarns of different counts. In this direction, a precise observation from Table 3 reveals that 20s 2-ply yarn shows maximum wicking than single yarn of the same count when tested individually as well as than the fabrics made out of these yarns as warp and weft respectively irrespective of warp, weft and diagonal way-wicking test. In the case of 20s 2-ply yarn, wicking height reaches up to 13.7 cm, whereas in warp-way fabric, wicking height reaches only up to 4.9 cm, the single yarn is in the intermediate height of 8.2 cm. Fabric wicking is reduced in comparison to yarn wicking for three reasons: yarn deformation in the fabric due to crimped condition, the number of interlacement in a unit length of a fabric sample and finally, the disruption of vertical wicking due to the occurrence of horizontal wicking at every point of interlacement. These characteristics can also be seen in twill weave fabrics. However, the effect is more or less the same as plain weave fabric considering the use of constituent coarser yarn in the fabric structure.
The maximum wicking height in 2 h for 30s 2-ply yarn is 10.7 cm, as indicated in Table 4, but when this yarn is present in fabric, the maximum warp-way wicking height is 5.7 cm in plain and 8.2 cm in a twill structure. The reason is the same as discussed before, but if we compare between plain weave fabric and twill weave fabric, the wicking height of twill weave fabric generates a higher value than that of the plain weave fabric. The explanation for this could be due to their fundamental design, as twill weave fabrics have less interlacements than plain weave fabrics. Another aspect we noticed from Table 4 is that twill weave fabric’s warp-way wicking reaches the height of 30s single yarn, which is not visible in plain weave fabric. The comparatively finer yarn composition could be the predominant factor for this behaviour.
The wicking behaviour of plain weave fabric is low when compared with both ply yarn and single yarn, as shown in Table 5, but when considering the twill weave, the wicking height in diagonal-way direction crosses the wicking height of warp-way direction, crosses the wicking height of single yarn and approaches the wicking height of ply yarn. This phenomenon might be caused by the angle of ply yarn and single yarn orientation in diagonal-way fabrics. The yarns are at a 45° angle in this orientation, which facilitates the wicking process rather than creating obstructions in the point of interlacement as observed in warp or weft-way fabrics. Moreover, it is observed that the fabric made of 40s 2-ply warp and 40s weft twill weave fabric has higher wicking height, which is may be due to the reason of higher porosity of the fabric woven from the finer yarns. As the cover factor is low in the finer fabric, which may be responsible for higher porosity, which confirms the same reported by Erdumlu and Saricam [42]. According to the capillary principle, smaller pores are filled first and influence the movement of the liquid. As the smaller pores are completely filled, the liquid moves to the larger pores [43].
6.2 The relationship between yarn wicking and fabric wicking in reference to different constituent yarns for various directions of plain and twill fabrics
The accompanying graphical figures (Figures 6–17) show the relationship between fabric wicking in various directions (warp, weft and diagonal) and its constituent yarn wicking (warp or weft) for plain and twill weave structures, from coarser to finer count. The first six graphical figures (Figures 6–11) are for plain weave fabrics only, while the remaining (Figures 12–17) are for twill weave fabrics. For all of these representations, a linear relationship is found to be the best fit, and the associated regression equation is also derived to establish the relationship.
Figure 6.
Relationship of wicking height between plain weave fabric (FP1) and constituent plied warp yarn (2/20s).
Figure 7.
Relationship of wicking height between plain weave fabric (FP1) and constituent single weft yarn (20s).
Figure 8.
Relationship of wicking height between plain weave fabric (FP2) and constituent plied warp yarn (2/30s).
Figure 9.
Relationship of wicking height between plain weave fabric (FP2) and constituent single weft yarn (30s).
Figure 10.
Relationship of wicking height between plain weave fabric (FP3) and constituent plied warp yarn (2/40s).
Figure 11.
Relationship of wicking height between plain weave fabric (FP3) and constituent single weft yarn (40s).
Figure 12.
Relationship of wicking height between twill weave fabric (FT1) and constituent plied warp yarn (2/20s).
Figure 13.
Relationship of wicking height between twill weave fabric (FT1) and constituent single weft yarn (20s).
Figure 14.
Relationship of wicking height between twill weave fabric (FT2) and constituent plied warp yarn (2/30s).
Figure 15.
Relationship of wicking height between twill weave fabric (FT2) and constituent single weft yarn (30s).
Figure 16.
Relationship of wicking height between twill weave fabric (FT3) and constituent plied warp yarn (2/40s).
Figure 17.
Relationship of wicking height between twill weave fabric (FT3) and constituent single weft yarn (40s).
Table 6 has a relationship matrix containing all of the regression equations (18 numbers) from Figures 4 to 9, expressing substantial evidence of a highly positive relationship between fabric wicking (y) and yarn wicking (x) for plain weave samples. The coefficient of determination (R2) is found to be in the range of 0.836–0.991, which means the coefficient of correlation values are almost closer to 1, which indicates that the proportion of variation is very low in the dependent variable that can be attributed to the independent variable within the range of experiments. The R2 values of the diagonal-way samples are between the R2 values of warp-way and weft-way samples composed of coarser to medium fineness yarns (20s and 30s), most likely due to the resultant effect of both the constituent plied warp and single weft yarns because the yarns are not in the direction in which the wicking has been measured. Regardless of warp or weft yarns, the relationship in a diagonal direction is found to be inferior for finer count (40s) fabric samples. As seen in Table 2, this result might be attributable to the lower fabric cover.
Parameters
Wicking height of plain weave fabric (cm)
Warp-way
Weft-way
Diagonal-way
Wicking height of 20s yarn (cm)
2-ply warp
y = 0.420x – 0.925 (R2 = 0.972)
y = 0.294x – 0.562 (R2 = 0.937)
y = 0.268x – 0.696 (R2 = 0.969)
Single weft
y = 0.713x – 1.289 (R2 = 0.973)
y = 0.508x – 0.864 (R2 = 0.968)
y = 0.457x – 0.938 (R2 = 0.976)
Wicking height of 30s yarn (cm)
2-ply warp
y = 0.709x – 2.478 (R2 = 0.966)
y = 0.390x – 1.147 (R2 = 0.990)
y = 0.393x – 1.403 (R2 = 0.981)
Single weft
y = 1.125x – 2.665 (R2 = 0.836)
y = 0.645x – 1.384 (R2 = 0.932)
y = 0.635x – 1.567 (R2 = 0.881)
Wicking height of 40s yarn (cm)
2-ply warp
y = 0.335x – 0.847 (R2 = 0.941)
y = 0.219x – 0.520 (R2 = 0.958)
y = 0.144x – 0.315 (R2 = 0.895)
Single weft
y = 0.695x – 1.082 (R2 = 0.985)
y = 0.452x – 0.664 (R2 = 0.991)
y = 0.335x – 0.847 (R2 = 0.941)
Table 6.
Matrices of regression equations and R2 values between fabric wicking and yarn wicking for plain weave fabric samples.
The correlation of wicking behaviour between fabrics of different directions (warp-way, weft-way and diagonal way) with respect to their constituent warp and weft yarns for twill weave samples is shown in a single representation using a similar relationship matrix derived from Figures 10–15 and arranged as Table 7. This table also aids in the identification of differences in relationship with plain weave samples of similar types as displayed in Table 6.
Parameters
Wicking height of twill fabric (cm)
Warp-way
Weft-way
Diagonal-way
Wicking height of 20s yarn (cm)
2-ply warp
y = 0.356x – 0.335 (R2 = 0.967)
y = 0.273x – 0.404 (R2 = 0.931)
y = 0.285x – 0.376 (R2 = 0.946)
Single weft
y = 0.610x – 0.671 (R2 = 0.982)
y = 0.473x – 0.696 (R2 = 0.970)
y = 0.492x – 0.671 (R2 = 0.979)
Wicking height of 30s yarn (cm)
2-ply warp
y = 0.877x – 2.085 (R2 = 0.974)
y = 0.687x – 1.466 (R2 = 0.987)
y = 0.685x – 1.691 R2 = 0.991
Single weft
y = 1.446x – 2.600 (R2 = 0.912)
y = 1.159x – 1.997 (R2 = 0.966)
y = 1.140x – 2.139 (R2 = 0.943)
Wicking height of 40s yarn (cm)
2-ply warp
y = 0.769x – 0.84 (R2 = 0.981)
y = 0.659x – 1.206 (R2 = 0.991)
y = 0.771x + 0.272 (R2 = 0.985)
Single weft
y = 1.526x – 1.114 (R2 = 0.939)
y = 1.331x – 1.528 (R2 = 0.982)
y = 1.539x – 0.036 (R2 = 0.954)
Table 7.
Matrices of regression equations and R2 values between fabric wicking and yarn wicking for twill weave fabric samples.
From the tabulated data of twill weave fabrics, the relationship of wicking between fabric and yarns is found to be much stronger (as the range of R2 lies within 0.912–0.991) compared with that of the plain weave in the fabric axis of the twill weave creating less amount of disturbance on capillary action due to the lower number of interlacements of twill design. As a result, the smooth movement of liquid within the yarn structure helps in a more effective wicking effect than plain weave structures, strengthening the relation between yarn and fabric wicking. As a result, regardless of the different directions of experimental fabric samples used in this investigation, changes in yarn fineness have a comparatively smaller impact on the connection [44].
7. Conclusion
The cotton fabrics presented in this chapter are only small fractions, which are produced globally for several applications. Absorbency and wicking are the key factors while producing or engineering a fabric for particular end uses such as sports, medical and other technical applications. Therefore, wickability of yarn and fabric has been studied critically as it is completely governed by their structure primarily. Therefore, even minor differences in structure can affect wicking height in both yarn and fabric. Increased fineness diminishes wickability in both ply and single yarn structures separately, but when employed in fabric structures, increased yarn fineness improves wicking [44]. Based on scientific experiments, uniquely presented correlation matrices have expressed the interrelation between cotton fabric and its constituent yarns showing strong correlation but varying nature due to differences in structure, direction of measurement, etc. Hence, these correlations can be used as a quick predictor of cotton fabric wicking based on the measured wicking of their constituent yarns for future research. Further research includes the study of absorbency and wicking with various solvents, temperature, and humidity for wide range of textile materials using these correlations with some modified equations.
Acknowledgments
The authors gratefully acknowledge the assistance provided by Prof. Sumanta Bhattacharya, Former Principal, and Prof. Biswapati Chatterjee, Former Head of the Department in Textile Technology, Government College of Engineering and Textile Technology, Serampore, West Bengal, India.
\n',keywords:"natural fibre, absorbency, wicking, capillary action, fabric structure",chapterPDFUrl:"https://cdn.intechopen.com/pdfs/80660.pdf",chapterXML:"https://mts.intechopen.com/source/xml/80660.xml",downloadPdfUrl:"/chapter/pdf-download/80660",previewPdfUrl:"/chapter/pdf-preview/80660",totalDownloads:56,totalViews:0,totalCrossrefCites:0,dateSubmitted:"November 23rd 2021",dateReviewed:"January 10th 2022",datePrePublished:"March 1st 2022",datePublished:null,dateFinished:"March 1st 2022",readingETA:"0",abstract:"In textiles of natural fibres, absorbency and wicking are considered as most indigenous liquid transmission properties, which play significant role in assessing the comfort of textile garments as well as in functioning of technical textiles. To explain the general principles of absorbency and wicking and their related parameters, a review of different theories is illustrated. Various structural aspects of textile intermediates such as yarn and fabric on wicking are discussed. An experimental analysis is also described to understand the wicking phenomena on fabrics in multiple directions such as warp-way, weft-way and diagonally for varying weave forms. A critical evaluation is presented for establish the wicking behaviour between these fabrics and their constituted yarns having preferred twisted forms such as single and ply. A unique representation of correlation matrices is shown to interrelate the yarn and fabric wicking.",reviewType:"peer-reviewed",bibtexUrl:"/chapter/bibtex/80660",risUrl:"/chapter/ris/80660",signatures:"Palash Mallick and Susanta Sekhar De",book:{id:"11122",type:"book",title:"Natural Fiber",subtitle:null,fullTitle:"Natural Fiber",slug:null,publishedDate:null,bookSignature:"Prof. Han-Yong Jeon",coverURL:"https://cdn.intechopen.com/books/images_new/11122.jpg",licenceType:"CC BY 3.0",editedByType:null,isbn:"978-1-80355-214-9",printIsbn:"978-1-80355-213-2",pdfIsbn:"978-1-80355-215-6",isAvailableForWebshopOrdering:!0,editors:[{id:"114618",title:"Prof.",name:"Han-Yong",middleName:null,surname:"Jeon",slug:"han-yong-jeon",fullName:"Han-Yong Jeon"}],productType:{id:"1",title:"Edited Volume",chapterContentType:"chapter",authoredCaption:"Edited by"}},authors:null,sections:[{id:"sec_1",title:"1. Introduction",level:"1"},{id:"sec_2",title:"2. Lucas-Washburn theory",level:"1"},{id:"sec_3",title:"3. Wetting",level:"1"},{id:"sec_3_2",title:"3.1 Wicking",level:"2"},{id:"sec_4_2",title:"3.2 Capillary theory",level:"2"},{id:"sec_6",title:"4. Liquid transport system",level:"1"},{id:"sec_6_2",title:"4.1 Wicking in yarn",level:"2"},{id:"sec_6_3",title:"4.1.1 Effect of yarn modification on water absorbency",level:"3"},{id:"sec_7_3",title:"4.1.2 Effect of yarn modification on wicking characteristics",level:"3"},{id:"sec_9_2",title:"4.2 Wicking in fabric",level:"2"},{id:"sec_9_3",title:"4.2.1 Effect of fabric parameters on wicking and its application as technical textiles",level:"3"},{id:"sec_12",title:"5. Experimental",level:"1"},{id:"sec_13",title:"6. Wicking behaviour of woven fabrics and its interrelation with their constituent yarns",level:"1"},{id:"sec_13_2",title:"6.1 Effect on wicking height (with respect to time) in various directions (warp-way, weft-way and diagonal-way) of fabrics as well as their constituent yarns",level:"2"},{id:"sec_14_2",title:"6.2 The relationship between yarn wicking and fabric wicking in reference to different constituent yarns for various directions of plain and twill fabrics",level:"2"},{id:"sec_16",title:"7. Conclusion",level:"1"},{id:"sec_17",title:"Acknowledgments",level:"1"}],chapterReferences:[{id:"B1",body:'Hsieh YL, Yu B, Hartzell MM. Liquid wetting, transport and retention properties of fibrous assemblies: Part II: Water wetting and retention of 100% and blended woven fabrics. Textile Research Journal. 1992;62(12):697-704. DOI: 10.1177/004051759206201201'},{id:"B2",body:'Ito H, Muraoka Y. Water transport along textile fibers as measured by an electrical capacitance technique. Textile Research Journal. 1993;63(2):414-420. DOI: 10.1177/004051759306300706'},{id:"B3",body:'Liu T. Coupled mechanical and liquid moisture transfer behaviour of textile materials [PhD thesis]. The Hong Kong Polytechnic University; 2008'},{id:"B4",body:'Banu KP. Wicking behaviour of fibres, yarns and fabrics [PhD thesis]. Mother Teresa Women’s University; 2013'},{id:"B5",body:'Washburn EW. The dynamics of capillary flow. Physical Review. 1921;17:273-283'},{id:"B6",body:'Pan N, Gibson P, editors. Thermal and Moisture Transport in Fibrous Materials. Cambridge, England: Woodhead Publishing Limited; 2006. pp. 136-153'},{id:"B7",body:'Hollies NRS, Kaessinger MM, Bogaty H. Water transport mechanisms in textile materials1 Part I: The role of yarn roughness in capillary-type penetration. Textile Research Journal. 1956;26:829-835. DOI: 10.1177/004051755602601102'},{id:"B8",body:'Hollies NRS, Kaessinger MM, Watson BS, Bogaty H. Water transport mechanisms in textile materials: Part II: Capillary-type penetration in yarns and fabrics. Textile Research Journal. 1957;27:8-13. DOI: 10.1177/004051755702700102'},{id:"B9",body:'Perwuelz A, Casetta M, Caze C. Liquid organisation during capillary rise in yarns—Influence of yarn torsion. Polymer Testing. 2001;20:553-561. DOI: 10.1016/S0142-9418(00)00075-1'},{id:"B10",body:'Liu T, Choi K, Li Y. Wicking in twisted yarns. Journal of Colloid and Interface Science. 2008;318:124-139'},{id:"B11",body:'Rajagopalan D, Aneja A. Modelling capillary flow in complex geometries. Textile Research Journal. 2001;71(9):813-821. DOI: 10.1177/004051750107100911'},{id:"B12",body:'Subramanian SN, Venkatachalam A, Subramaiam V. Wicking behaviour of regular ring, jet ring-spun and other types of compact yarns. Indian Journal of Fibre and Textile Research. 2007;32:158-162'},{id:"B13",body:'Wang N, Zha A, Wang J. Study on the wicking property of polyester filament yarns. Fibers and Polymers. 2008;9(1):97-100. DOI: 10.1007/s12221-008-0016-2'},{id:"B14",body:'De SS, Mallick P. Study the wicking characteristics of cotton yarns. In: 3rd National Conference on Emerging Trends in Textiles, Fibre and Apparel Engineering. Berhampore, India: Department of Textile Technology, Government College of Engineering and Textile Technology; 2016. pp. 8-12'},{id:"B15",body:'De SS, Porel S, Patra N, Kundu B, Mallick P. Influence of different cotton yarn structures on wicking characteristics. American International Journal of Research in Sciences, Technology, Engineering and Mathematics. 2016;15(2):173-176'},{id:"B16",body:'Das A, Ishtiaque SM, Yadav P. Properties of woven fabrics containing core-sheath DREF-III yarn in weft. Indian Journal of Fibre and Textile Research. 2003;28:260-264'},{id:"B17",body:'Montgomery DC. Design & Analysis of Experiments. 8th ed. Vol. 5. Singapore: John Wiley & Sons; 2004. p. 427'},{id:"B18",body:'Walker Esq EM, FTI, Doyle PJ. Some fundamental properties of hosiery yarns and their relation to the mechanical characteristics of knitted fabrics. Journal of the Textile Institute. 1952;43(1):19-35. DOI: 10.1080/19447015208663954'},{id:"B19",body:'Merati AA, Okamura M. Hollow yarn in friction spinning: part I: tensile properties of hollow yarn. Textile Research Journal. 2000;70(12):1070-1076. DOI: 10.1177/004051750007001206'},{id:"B20",body:'Slater K. Comfort properties of textile. Textile Progress. 1977;9(4):1-70. DOI: 10.1080/00045167.1977.10750095'},{id:"B21",body:'Knapton JJF, Truter EV, Aziz AKMA. The geometry, dimensional properties, and stabilization of the cotton plain-jersey structure. Journal of the Textile Institute. 1975;66(12):413-419. DOI: 10.1080/00405007508630536'},{id:"B22",body:'Postle R. A geometrical assessment of the thickness and bulk density of weft-knitted fabrics. Journal of the Textile Institute. 1974;65(4):155-163. DOI: 10.1080/00405007408630442'},{id:"B23",body:'Lord PR. Handbook of Yarn Production. Cambridge: Woodhead Publishing Ltd.; 2003'},{id:"B24",body:'Yoo HS, Hu YS, E A K. Effects of heat and moisture transport in fabrics and garments determined with a vertical plate sweating skin model. Textile Research Journal. 2000;70(6):542-549. DOI: 10.1177/004051750007000612'},{id:"B25",body:'Ansari N, Haghighat Kish M. The wicking of water in yarn as measured by an electrical resistance technique. Journal of the Textile Institute. 2000;91(3):410-419. DOI: 10.1080/00405000008659517'},{id:"B26",body:'Das A, Ishtiaque SM. Comfort characteristics of fabrics containing twist-less and hollow fibrous assemblies in weft. Journal of Textile and Apparel, Technology and Management. 2004;3(4):1-7'},{id:"B27",body:'Anbahan Ariadurai S, Prasad P, Whyte IL. Modeling the in-plane permeability of woven geotextiles. Textile Research Journal. 1999;69(5):345-351. DOI: 10.1177/004051759906900507'},{id:"B28",body:'Kissa E. Wetting and wicking. Textile Research Journal. 1996;66(10):660-668. DOI: 10.1177/004051759606601008'},{id:"B29",body:'Roy MD, Chattopadhayay R, Sinha SK. Wicking performance of profiled fibre. Part B: Assessment of fabrics. Journal of The Institution of Engineers (India): Series E. 2018;99:1-8'},{id:"B30",body:'Ramesh Babu V, Ramakrishnan G, Subramaniam VS, Lakshmi K. Influence of the weave factor on the character of fabric wicking measured by a multiple probe vertical wicking tester. Fibres & Textiles in Eastern Europe. 2011;19(5,88):60-63'},{id:"B31",body:'Chattopadhyay R. One Day Seminar on Comfort in Textile. Delhi: Department of Textile Technology, IIT; 2004. p. 20'},{id:"B32",body:'Sharma N, Kumar P, Bhatia D, Sinha SK. Moisture management behaviour of knitted fabric from structurally modified ring and vortex spun yarn. Journal of The Institution of Engineers (India): Series E. 2016;97:123-129'},{id:"B33",body:'Mallick P, De SS. Study the wicking phenomena in different directions of cotton plain and twill fabrics made of variable yarn counts. In: International Conference in Textile and Clothing-Present and Future Trends. Kolkata, India: Department of Jute and Fibre Technology, University of Calcutta; 2017. pp. 75-79'},{id:"B34",body:'Zhu G, Militky J, Wang Y, Sunderlal BV, Kremenokova D. Study on the wicking property of cotton fabric. Fibres & Textiles in Eastern Europe. 2015;23(2(110)):137-140'},{id:"B35",body:'Ozdemir H. Permeability and wicking properties of modal and lyocell woven fabrics used for clothing. Journal of Engineered Fibers and Fabrics. 2017;12(1):12-21. DOI: 10.1177/155892501701200102'},{id:"B36",body:'Bhargava GS. Effect of kind of terry weave on strength, water absorbency and wettability of terry fabrics. Indian Textile Journal. 1985;95(9):95-101'},{id:"B37",body:'Anand SC, Higgins L. Textile materials and products for activewear and sportwear. In: 2nd International Conference of NISTI, New Delhi, India. 2–3 December 2004. p. 204'},{id:"B38",body:'Silva APD, Anand SC. Responsive garments for sportswear. In: Proceedings on Smart Textile, NIFT, New Delhi, India. 29 November 2000. p. 32'},{id:"B39",body:'Ishtiaque SM. One Day Seminar on Automotive Textiles, SASMIRA, Mumbai, India. 19 February 2000. p. 67'},{id:"B40",body:'Patnaik A, Rengasamy RS, Kothari VK, Ghosh A. Wetting and Wicking in Fibrous Materials, Textile Progress. Manchester: The Textile Institute; 2010'},{id:"B41",body:'Sanyal T. Jute geotextiles: Its types and functions. In: Jute Geotextiles and their Applications in Civil Engineering. Singapore: Springer; 2017. pp. 19-31. DOI: 10.1007/978-981-10-1932-6_3'},{id:"B42",body:'Erdumlu N, Saricam C. Wicking and drying properties of conventional ring and vortex-spun cotton yarns and fabrics. Journal of the Textile Institute. 2013;104(12):1284-1291. DOI: 10.1080/00405000.2013.799258'},{id:"B43",body:'Wong KK, Tao XM, Yuen CWM, Yeung KW. Wicking properties of linen treated with low temperature plasma. Textile Research Journal. 2001;71(1):49-56. DOI: 10.1177/004051750107100108'},{id:"B44",body:'Mallick P, De SS. Study the wicking phenomena of cotton woven fabrics and its constituent yarns: Relation between fabric wicking and yarn wicking. Journal of Natural Fibers. 2021. DOI: 10.1080/15440478.2021.1875371'}],footnotes:[],contributors:[{corresp:"yes",contributorFullName:"Palash Mallick",address:"palashmallick91@gmail.com",affiliation:'
Department of Jute and Fibre Technology, University of Calcutta, India
Department of Textile Technology, Government College of Engineering and Textile Technology, India
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Hair is a derivative of the epidermis and consists of two distinct parts: the follicle and the hair shaft. The follicle is the essential unit for the generation of hair. The hair shaft consists of a cortex and cuticle cells, and a medulla for some types of hairs. Hair follicle has a continuous growth and rest sequence named hair cycle. The duration of growth and rest cycles is coordinated by many endocrine, vascular and neural stimuli and depends not only on localization of the hair but also on various factors, like age and nutritional habits. Distinctive anatomy and physiology of hair follicle are presented in this chapter. Extensive knowledge on anatomical and physiological aspects of hair can contribute to understand and heal different hair disorders.",book:{id:"5461",slug:"hair-and-scalp-disorders",title:"Hair and Scalp Disorders",fullTitle:"Hair and Scalp Disorders"},signatures:"Bilgen Erdoğan",authors:[{id:"193661",title:"Dr.",name:"Bilgen",middleName:null,surname:"Erdoğan",slug:"bilgen-erdogan",fullName:"Bilgen Erdoğan"}]},{id:"52801",doi:"10.5772/66156",title:"Psychosocial Aspects of Hair Loss",slug:"psychosocial-aspects-of-hair-loss",totalDownloads:2523,totalCrossrefCites:6,totalDimensionsCites:7,abstract:"Hair loss (alopecia) is a common dermatological condition that affects men and women of all ages. It can be due to a wide variety of causes including scarring and non-scarring diseases. Although alopecia is not a life-threatening condition, it has significant psychological impact on the quality of life. Mental disorders such as anxiety, depression, social phobia, posttraumatic stress disorder, and suicidal thoughts are increased among alopecia patients. On the other hand, alopecia frequency increases during the course of psychological disorders. In this chapter, psychosocial aspects of hair loss and the relationship between alopecia and psychological disorders are reviewed.",book:{id:"5461",slug:"hair-and-scalp-disorders",title:"Hair and Scalp Disorders",fullTitle:"Hair and Scalp Disorders"},signatures:"Hilal Gokalp",authors:[{id:"193580",title:"M.D.",name:"Hilal",middleName:null,surname:"Gokalp",slug:"hilal-gokalp",fullName:"Hilal Gokalp"}]},{id:"62733",doi:"10.5772/intechopen.79807",title:"Ethosomes: An Exciting and Promising Alcoholic Carrier System for Treating Androgenic Alopecia",slug:"ethosomes-an-exciting-and-promising-alcoholic-carrier-system-for-treating-androgenic-alopecia",totalDownloads:1073,totalCrossrefCites:1,totalDimensionsCites:5,abstract:"Androgenetic alopecia (male-pattern hair loss) is characterized by the deposition of dihydrotestosterone at the pilosebaceous unit of the scalp. Oral administration of drugs (like finasteride) which can reverse androgenic alopecia causes undesired effects to the body. Targeting these drugs directly to the pilosebaceous unit of the scalp will enhance the pharmacological response at the desired site by reducing undesired systemic side effects. This chapter discusses about ethosomes, a specially tailored ethanolic vesicular carriers which can efficiently deliver various drugs with different physicochemical properties to and through the skin. The unique characteristics of the ethosomal carriers, their composition, preparation methods, and the mechanism of permeation, safety, and practical experience (finasteride and herbal extracts) have been discussed in detail.",book:{id:"6961",slug:"alopecia",title:"Alopecia",fullTitle:"Alopecia"},signatures:"Veintramuthu Sankar, Santhanam Ramesh and Karthik Siram",authors:[{id:"254541",title:"Prof.",name:"Sankar",middleName:null,surname:"Veintramuthu",slug:"sankar-veintramuthu",fullName:"Sankar Veintramuthu"},{id:"260986",title:"Mr.",name:"Karthik",middleName:null,surname:"Siram",slug:"karthik-siram",fullName:"Karthik Siram"},{id:"260991",title:"Dr.",name:"Santhanam",middleName:null,surname:"Ramesh",slug:"santhanam-ramesh",fullName:"Santhanam Ramesh"}]},{id:"54160",doi:"10.5772/66747",title:"Cosmetic Procedures in the Treatment of Alopecia",slug:"cosmetic-procedures-in-the-treatment-of-alopecia",totalDownloads:3364,totalCrossrefCites:1,totalDimensionsCites:3,abstract:"Alopecia has a significant negative impact on the quality of life. Unfortunately, there is no satisfactory cure for most types of alopecia. Alopecia is divided into cicatricial and noncicatricial types. Androgenetic alopecia, alopecia areata, and telogen effluvium are common forms of noncicatricial alopecias. In order to treat or improve the appearance, various procedures that are being applied for different types of alopecia including mesotherapy, microneedling, platelet‐rich plasma, low‐level light therapy, and stem‐cell therapy with variable outcomes are reviewed in this chapter.",book:{id:"5461",slug:"hair-and-scalp-disorders",title:"Hair and Scalp Disorders",fullTitle:"Hair and Scalp Disorders"},signatures:"Selda Pelin Kartal, Cemile Altunel and Bilgen Gencler",authors:[{id:"72686",title:"Prof.",name:"Selda Pelin",middleName:null,surname:"Kartal",slug:"selda-pelin-kartal",fullName:"Selda Pelin Kartal"}]}],mostDownloadedChaptersLast30Days:[{id:"53880",title:"Anatomy and Physiology of Hair",slug:"anatomy-and-physiology-of-hair",totalDownloads:7757,totalCrossrefCites:5,totalDimensionsCites:8,abstract:"Hair is one of the characteristic features of mammals and has various functions such as protection against external factors; producing sebum, apocrine sweat and pheromones; impact on social and sexual interactions; thermoregulation and being a resource for stem cells. Hair is a derivative of the epidermis and consists of two distinct parts: the follicle and the hair shaft. The follicle is the essential unit for the generation of hair. The hair shaft consists of a cortex and cuticle cells, and a medulla for some types of hairs. Hair follicle has a continuous growth and rest sequence named hair cycle. The duration of growth and rest cycles is coordinated by many endocrine, vascular and neural stimuli and depends not only on localization of the hair but also on various factors, like age and nutritional habits. Distinctive anatomy and physiology of hair follicle are presented in this chapter. Extensive knowledge on anatomical and physiological aspects of hair can contribute to understand and heal different hair disorders.",book:{id:"5461",slug:"hair-and-scalp-disorders",title:"Hair and Scalp Disorders",fullTitle:"Hair and Scalp Disorders"},signatures:"Bilgen Erdoğan",authors:[{id:"193661",title:"Dr.",name:"Bilgen",middleName:null,surname:"Erdoğan",slug:"bilgen-erdogan",fullName:"Bilgen Erdoğan"}]},{id:"53947",title:"Infections, Infestations and Neoplasms of the Scalp",slug:"infections-infestations-and-neoplasms-of-the-scalp",totalDownloads:3472,totalCrossrefCites:0,totalDimensionsCites:0,abstract:"This chapter reviews common cutaneous infections, infestations, and neoplasms of the scalp. Infections of the scalp are subdivided into three major groups. The most seen are: (1) Bacterial: Folliculitis, folliculitis decalvans, tufted hair folliculitis and acne keloidalis nuchae. (2) Fungal: Tinea capitis, favus and kerion celsi. (3) Protozoal: Syphilitic alopecia. Pediculosis capitis is the most common worldwide infestation of the scalp. The neoplasms of the scalp are large group of different diseases due to arising different origin. In the following section, trichilemmal cyst, proliferating trichilemmal cyst, nevus sebaceous and cylindroma are discussed in detail.",book:{id:"5461",slug:"hair-and-scalp-disorders",title:"Hair and Scalp Disorders",fullTitle:"Hair and Scalp Disorders"},signatures:"Filiz Canpolat",authors:[{id:"191617",title:"Associate Prof.",name:"Filiz",middleName:null,surname:"Canpolat",slug:"filiz-canpolat",fullName:"Filiz Canpolat"}]},{id:"53525",title:"Trichoscopy and Trichogram",slug:"trichoscopy-and-trichogram",totalDownloads:2605,totalCrossrefCites:0,totalDimensionsCites:0,abstract:"Hair and scalp examination techniques can be classified into three categories: noninvasive methods (clinical history, general examination, photography, hair count, weighing shed hair, pull test, global hair counts, dermoscopy, electron microscopy, laser scanning microscopy, etc.); semi‐invasive methods (the trichogram, unit areatrichogram); and invasive methods (biopsies in cicatritial alopecia). Scalp dermoscopy or trichoscopy is one of thenoninvasive techniques for the evaluation of patients with hair loss that allows for magnified visualization of the hair and scalp skin. It may be performed with a manual dermoscope (10× magnification) or a videodermoscope (up to 1000× magnification). This method is simple, quick, and easy to perform, is well‐accepted by patients, and is useful for monitoring treatment, determining severity of the disease and follow‐up. It is a simple, minimally invasive and rapid technique for measuring hair follicle activity. Trichogram represents a semi‐invasive technique for the evaluation of patients with hair loss that allows the microscopic examination of hairs plucked from the scalp and provides information about the state of the proximal end of the hair shaft and the distal end. The trichogram is a useful complementary tool for clinical evaluation, diagnosis, and the monitoring of treatment response.",book:{id:"5461",slug:"hair-and-scalp-disorders",title:"Hair and Scalp Disorders",fullTitle:"Hair and Scalp Disorders"},signatures:"Melike Kibar",authors:[{id:"189899",title:"Dr.",name:"Melike",middleName:null,surname:"Kibar Ozturk",slug:"melike-kibar-ozturk",fullName:"Melike Kibar Ozturk"}]},{id:"42524",title:"Hereditary Palmoplantar Keratosis",slug:"hereditary-palmoplantar-keratosis",totalDownloads:4540,totalCrossrefCites:0,totalDimensionsCites:0,abstract:null,book:{id:"3038",slug:"current-genetics-in-dermatology",title:"Current Genetics in Dermatology",fullTitle:"Current Genetics in Dermatology"},signatures:"Tamihiro Kawakami",authors:[{id:"155091",title:"Associate Prof.",name:"Tamihiro",middleName:null,surname:"Kawakami",slug:"tamihiro-kawakami",fullName:"Tamihiro Kawakami"}]},{id:"63066",title:"Pharmacological Treatment of Alopecia",slug:"pharmacological-treatment-of-alopecia",totalDownloads:1434,totalCrossrefCites:1,totalDimensionsCites:2,abstract:"In this chapter, we will explore non-surgical treatments of alopecia. Unlike many other areas of medicine, pharmacological treatments for alopecia are relatively new. There are only two treatments which are approved by the Food and Drug Administration (FDA); the rest are drugs developed for other indications which have gained popular off-label use to promote hair growth. The reasons for this are many, including the designation of alopecia by the FDA as a cosmetic disease. This designation has restricted alopecia development programs to compounds with virtually no side effects. Unfortunately, it has also led to off-label use of far more dangerous compounds as alopecia treatments, without the benefit of controlled trials. There is a growing recognition that alopecia, particularly alopecia areata and chemotherapy-induced alopecia, are disorders which significantly alter the quality of life, similar to acne vulgaris and psoriasis, and merit treatment accordingly. There have also been several recent advances in our understanding of the hair cycle, revealing new targets for developing alopecia therapies. As a result, there is a more robust slate of programs for developing new pharmacological treatments for alopecia. 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He is a full professor of signal processing and pattern recognition and is head of the Signals and Communications Department at ULPGC, teaching from 2001 on subjects on signal processing and learning theory. His research lines are biometrics, biomedical signals and images, data mining, classification system, signal and image processing, machine learning, and environmental intelligence. He has researched in 52 international and Spanish research projects, some of them as head researcher. He is co-author of 4 books, co-editor of 27 proceedings books, guest editor for 8 JCR-ISI international journals, and up to 24 book chapters. He has over 450 papers published in international journals and conferences (81 of them indexed on JCR – ISI - Web of Science). He has published seven patents in the Spanish Patent and Trademark Office. He has been a supervisor on 8 Ph.D. theses (11 more are under supervision), and 130 master theses. 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His research interests include computer/machine vision, machine learning, pattern recognition, computational intelligence. \nDr. Papakostas served as a reviewer in numerous journals, as a program\ncommittee member in international conferences and he is a member of the IAENG, MIR Labs, EUCogIII, INSTICC and the Technical Chamber of Greece (TEE).",institutionString:null,institution:{name:"International Hellenic University",institutionURL:null,country:{name:"Greece"}}},editorTwo:null,editorThree:null},{id:"25",title:"Evolutionary Computation",coverUrl:"https://cdn.intechopen.com/series_topics/covers/25.jpg",isOpenForSubmission:!0,editor:{id:"136112",title:"Dr.",name:"Sebastian",middleName:null,surname:"Ventura Soto",slug:"sebastian-ventura-soto",fullName:"Sebastian Ventura Soto",profilePictureURL:"https://mts.intechopen.com/storage/users/136112/images/system/136112.png",biography:"Sebastian Ventura is a Spanish researcher, a full professor with the Department of Computer Science and Numerical Analysis, University of Córdoba. 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He is currently a principal researcher in data analytics and optimisation at TECNALIA (Spain), a visiting fellow at the Basque Center for Applied Mathematics (BCAM) and a part-time lecturer at the University of the Basque Country (UPV/EHU). His research interests gravitate on the use of descriptive, prescriptive and predictive algorithms for data mining and optimization in a diverse range of application fields such as Energy, Transport, Telecommunications, Health and Industry, among others. In these fields he has published more than 240 articles, co-supervised 8 Ph.D. theses, edited 6 books, coauthored 7 patents and participated/led more than 40 research projects. 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He is currently a full professor in\nthe Department of Automation and Applied Informatics at the\nsame university. Dr. Voloşencu is the author of ten books, seven\nbook chapters, and more than 160 papers published in journals\nand conference proceedings. He has also edited twelve books and\nhas twenty-seven patents to his name. He is a manager of research grants, editor in\nchief and member of international journal editorial boards, a former plenary speaker, a member of scientific committees, and chair at international conferences. His\nresearch is in the fields of control systems, control of electric drives, fuzzy control\nsystems, neural network applications, fault detection and diagnosis, sensor network\napplications, monitoring of distributed parameter systems, and power ultrasound\napplications. 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