CN110241602B - Spiral grating density disc and method for measuring warp and weft density of fabric - Google Patents
Spiral grating density disc and method for measuring warp and weft density of fabric Download PDFInfo
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Abstract
Description
技术领域technical field
本发明属于测量设备技术领域,具体涉及一种螺线光栅密度盘及织物经纬密度的测量方法。The invention belongs to the technical field of measuring equipment, and particularly relates to a spiral grating density disc and a method for measuring the warp and weft density of fabrics.
背景技术Background technique
纺织品的经纬密度通常指每厘米或每英寸长(宽)度内经纱或纬纱的条数(国内标准也常表示为10cm内纱线条数)。密度的大小,直接影响织物的外观、手感、厚度、强力、抗折性、透气性、耐磨性和保暖性能等物理机械指标,同时他也关系到产品的成本和生产效率的高低。现有测量织物经纬密度的主要方法有:(1)织物分解法:即分解规定尺寸的织物后人工数出纱线条数。(2)移动式织物密度镜法:即使用移动式织物密度镜,将织物在视野中放大后数出一定长度内纱线条数,再折算至10cm。(3)计算机软件模拟分析法:通过计算机成像与图像识别技术模拟织物表面结构来计算经纬密度。(4)斜线光栅测定法:将斜线光栅密度镜(密度仪)放置在织物上,转至纱线方向时将显示类似菱形的多组反比例曲线对称花纹,其尖角所指位置处刻度数即代表经向(或纬向)密度数。以上前三种方法测量精确度较高,但配置仪器或人工成本很高,测量速度也较慢。第四种方法虽然仪器和人工成本低,但斜线光栅上刻度为非均匀刻度,并且出现的莫尔条纹分布复杂而分散,不易对准读数位置,因而测量精确度较低。即现有测量方法精确度与测量成本间有较大矛盾。The warp and weft density of textiles usually refers to the number of warp or weft yarns per centimeter or per inch of length (width) (the domestic standard is often expressed as the number of yarns within 10cm). The size of the density directly affects the physical and mechanical indicators such as the appearance, feel, thickness, strength, folding resistance, air permeability, wear resistance and thermal insulation performance of the fabric, and it is also related to the cost of the product and the level of production efficiency. The existing main methods for measuring the warp and weft density of fabrics are as follows: (1) Fabric decomposition method: that is, manually count the number of yarns after decomposing a fabric of a specified size. (2) Mobile fabric density mirror method: that is, using a mobile fabric density mirror, after magnifying the fabric in the field of view, count the number of yarns in a certain length, and then convert it to 10cm. (3) Computer software simulation analysis method: The warp and weft density is calculated by simulating the fabric surface structure through computer imaging and image recognition technology. (4) Slanted grating measurement method: Place the slanted grating densitometer (densitometer) on the fabric and turn to the yarn direction to display multiple sets of symmetrical patterns of inversely proportional curves similar to rhombus, and the scale at the position pointed by the sharp corner The number represents the warp (or weft) density number. The first three methods above have high measurement accuracy, but the cost of configuring instruments or labor is high, and the measurement speed is also slow. Although the fourth method has low instrument and labor costs, the scale on the slanted grating is non-uniform, and the moiré fringe distribution that appears is complex and scattered, and it is not easy to align the reading position, so the measurement accuracy is low. That is, there is a great contradiction between the accuracy of the existing measurement methods and the measurement cost.
发明内容SUMMARY OF THE INVENTION
针对现有技术中的缺陷和不足,本发明提供了一种螺线光栅密度盘及织物经纬密度的测量方法,克服现有的织物经纬密度测量方法存在测量精度低、测量成本很高等缺陷。Aiming at the defects and deficiencies in the prior art, the present invention provides a spiral grating density disc and a method for measuring the warp and weft density of fabrics, which overcome the defects of low measurement accuracy and high measurement cost in the existing fabric warp and weft density measurement methods.
为达到上述目的,本发明采取如下的技术方案:To achieve the above object, the present invention adopts the following technical scheme:
本发明提供一种螺线光栅密度盘,包括透明基板,在所述透明基板上制有多条均绕同一中心原点逆时针旋转而成的反比例螺旋线形的光栅线;在逆时针旋转过程中,每条所述光栅线的矢径长度均逐渐减小;位于最中心的光栅线的旋转角度是360度,且其他各条光栅线的旋转角度等于或小于360度;在所述透明基板还设有与光栅线同心的多圈刻度圆周,刻度圆周外侧标定有垂直于刻度圆周的直线刻度线;The invention provides a helical grating density disk, comprising a transparent substrate, on which a plurality of inversely proportional helical grating lines are formed by rotating counterclockwise around the same central origin; during the counterclockwise rotation, The radial vector length of each grating line gradually decreases; the rotation angle of the grating line at the center is 360 degrees, and the rotation angle of the other grating lines is equal to or less than 360 degrees; There is a multi-circle scale circle concentric with the grating line, and a straight line scale line perpendicular to the scale circle is marked on the outside of the scale circle;
所述螺线光栅密度盘与织物重叠并相对转动时,会显示出一条沿矢径方向的直线读数条纹,该直线读数条纹在对应刻度圆周上所指刻度值即为织物经纱密度或纬纱密度。When the helical grating density disc overlaps with the fabric and rotates relatively, it will display a linear reading stripe along the radial direction, and the scale value indicated by the linear reading stripe on the corresponding scale circle is the fabric warp density or weft density.
本发明还包括如下技术特征:The present invention also includes the following technical features:
具体的,所述光栅线在极坐标系中满足以下方程:其中,ρ为矢径长度,即光栅线上任一点与中心原点连线的长度;n为光栅线序号,从中心原点到边缘依次取值为n=1,2,3,…;θ为极角,是矢径相对极轴逆时针旋转转过的角度(也即矢径与极轴的夹角),θ取值在长度为2π的区间[θ1,θ2]内,θ1为最小极角,θ2=θ1+2π为最大极角;a为长度量,决定光栅线上各点矢径长度和相邻光栅线在同一极角方向上对应点矢径长度之差(即相邻光栅线在该极角方向上对应点的距离),并与最小极角θ1共同决定螺线光栅密度盘的量程。Specifically, the grating lines satisfy the following equation in the polar coordinate system: Among them, ρ is the length of the vector radius, that is, the length of the line connecting any point on the grating line and the central origin; n is the serial number of the grating line, which is n=1, 2, 3, ... in order from the central origin to the edge; θ is the polar angle , is the counterclockwise rotation angle of the vector radius relative to the polar axis (that is, the angle between the vector radius and the polar axis ) . Angle, θ 2 =θ 1 +2π is the maximum polar angle; a is the length, which determines the difference between the length of each point on the grating line and the length of the corresponding point on the adjacent grating line in the same polar angle direction (that is, adjacent The distance between the grating lines in the polar angle direction corresponds to the point), and together with the minimum polar angle θ 1 determines the range of the helical grating density disk.
具体的,所述刻度圆周有两条,分别为内圈刻度圆周和外圈刻度圆周,在内圈刻度圆周和外圈刻度圆周之间还设有同心的圆形线;Specifically, there are two scale circles, which are the inner circle scale circle and the outer circle scale circle, and a concentric circular line is also provided between the inner circle scale circle and the outer circle scale circle;
所述内圈刻度圆周的半径为R,根据R值能得到内圈刻度圆周之内的光栅线的序号取值范围;The radius of the scale circle of the inner ring is R, and the value range of the serial number of the grating line within the scale circle of the inner ring can be obtained according to the R value;
所述外圈刻度圆周的半径为R2,所述圆形线的半径为R1,所述外圈刻度圆周和圆形线之间为位于环带内的光栅线,根据R1和R2值能得到位于环带内的光栅线的序号取值范围。The radius of the scale circle of the outer ring is R 2 , the radius of the circular line is R 1 , and between the scale circle of the outer ring and the circular line is a grating line located in the annular zone, according to R 1 and R 2 The value can get the range of the serial number of the raster line located in the annular band.
具体的,各光栅线在同一极角方向上的对应点的矢径长度构成等差数列,即任意两条相邻的光栅线在同一极角方向上的对应点间距相等,都为与极角θ成反比,具有空间周期性。Specifically, the radii lengths of the corresponding points of each grating line in the same polar angular direction constitute an arithmetic sequence, that is, the corresponding points of any two adjacent grating lines in the same polar angular direction have the same spacing, both of which are It is inversely proportional to the polar angle θ and has spatial periodicity.
具体的,所述光栅线的自身宽度随极角变化,在任一极角方向上的宽度都相等,等于相邻光栅线在该极角方向上的对应点间距。Specifically, the self-width of the grating lines varies with the polar angle, and the widths in any polar angle direction are equal, which is equal to the corresponding point spacing of adjacent grating lines in the polar angle direction.
具体的,所述刻度圆周上刻度线的分布规律满足方程:其中,D为刻度值;所述刻度值为公制或英制,单位为线数/厘米或线数/英寸;Specifically, the distribution law of the scale lines on the scale circle satisfies the equation: Wherein, D is the scale value; the scale value is metric or imperial, and the unit is lines/cm or lines/inch;
所述刻度值的最小刻度值为D1,最大刻度值为D2,分别对应光栅线的最小极角θ1和最大极角θ2;其中,The minimum scale value of the scale value is D 1 , and the maximum scale value is D 2 , respectively corresponding to the minimum polar angle θ 1 and the maximum polar angle θ 2 of the grating line; wherein,
具体的,所述刻度圆周上刻度线的分布规律方程的公式推导如下:Specifically, the distribution law equation of the scale lines on the scale circle The formula is derived as follows:
当θ=θ0为任一固定数值时,序号为n的光栅线在极角θ0方向上对应点的矢径长度为即该点极坐标为相邻两条光栅线的矢径长度之差为常量 When θ=θ 0 is any fixed value, the radial vector length of the corresponding point of the grating line with serial number n in the direction of polar angle θ 0 is That is, the polar coordinates of the point are The difference between the radial lengths of two adjacent raster lines is constant
曲线L1为所述光栅线,直线L2为极角θ0方向的矢径,直线L3为各光栅线在极角θ0方向的对应点处的切线,直线L4为与各切线垂直的法线方向的矢径;The curve L1 is the grating line, the straight line L2 is the vector radius in the direction of the polar angle θ 0 , and the straight line L3 is the corresponding point of each grating line in the direction of the polar angle θ 0 The tangent at , the straight line L4 is the vector radius of the normal direction perpendicular to each tangent;
直线L4与极轴夹角为φ,直线L4与直线L2夹角为φ-θ0,直线L3与直线L2的夹角为α; The included angle between the straight line L4 and the polar axis is φ, the included angle between the straight line L4 and the straight line L2 is φ-θ 0 , and the included angle between the straight line L3 and the straight line L2 is α;
光栅线上一点处的切线方程为ρcos(θ-φ)=nd,其中,n为切线序号,也为光栅线序号;A point on the raster line The tangent equation at is ρcos(θ-φ)=nd, where n is the serial number of the tangent, which is also the serial number of the grating line;
所述切线均互相平行且等间距,切线斜率均为该斜率与n值无关;d为相邻两条切线之间的距离,螺线光栅密度盘与织物相对转动,直至光栅线的切线与织物的纱线重合时,得到纱线密度 The tangents are all parallel to each other and are equally spaced, and the slopes of the tangents are The slope is independent of the value of n; d is the distance between two adjacent tangents, The helical grating density disc rotates relative to the fabric until the tangent of the grating line coincides with the yarn of the fabric to obtain the yarn density
具体的,当织物经纱间距等于θ0方向上光栅线对应点处的切线的间距时,使螺线光栅密度盘与织物相对转动,直至光栅线的切线与织物的纱线重合,则该θ0方向上莫尔条纹空间频率为零,即莫尔条纹间距无穷大;则此处出现一条沿θ0方向无限延伸的较宽的明条纹,即直线读数条纹;直线读数条纹在对应刻度圆周上所指刻度值即为织物经纱或纬纱密度。Specifically, when the warp distance of the fabric is equal to the corresponding point of the grating line in the direction of θ 0 When the distance between the tangent lines at
具体的,可根据实际量程标定刻度;Specifically, according to the actual range calibration scale;
即量程下限为上限为 That is, the lower limit of the range is capped at
可算出θ1为下限D1对应极角,θ1+2π为上限D2对应极角;根据此a和θ1能画出光栅线。can be calculated θ 1 is the polar angle corresponding to the lower limit D 1 , and θ 1 +2π is the polar angle corresponding to the upper limit D 2 ; according to this a and θ 1 , the grating line can be drawn.
本发明还提供一种织物经纬密度的测量方法,该测量方法采用所述的螺线光栅密度盘进行测量,该测量方法的步骤如下:The present invention also provides a method for measuring the warp and weft density of fabrics. The measuring method adopts the spiral grating density disc to measure, and the steps of the measuring method are as follows:
步骤一:将所述螺线光栅密度盘覆盖在织物上,初始在近似垂直于织物经纱(或纬纱)方向附近会出现多条弯曲的明暗相间的条纹;Step 1: Cover the helical grating density disk on the fabric, and initially there will be a plurality of curved light and dark stripes near the direction approximately perpendicular to the warp (or weft) of the fabric;
步骤二:然后转动所述螺线光栅密度盘,使弯曲的条纹数逐渐减少,直至最终只显示为一条沿矢径方向的较宽明条纹,即直线读数条纹,该直线读数条纹在刻度圆周上所指刻度值即为织物经纱密度或纬纱密度。Step 2: Then turn the helical grating density disk to gradually reduce the number of curved fringes, until finally only a wider bright fringe along the radial direction is displayed, that is, a straight reading fringe, which is on the scale circle. The scale value referred to is the fabric warp density or weft density.
本发明与现有技术相比,有益的技术效果是:Compared with the prior art, the present invention has the following beneficial technical effects:
(Ⅰ)本发明的螺线光栅密度盘与织物重叠并相对转动时,会显示出一条沿矢径方向的直线读数条纹,该直线读数条纹在刻度圆周上所指刻度值即为织物经纱密度或纬纱密度,可以快速方便地测量织物经纬密度,同时也能保证较高的精确度。(I) When the helical grating density disc of the present invention overlaps with the fabric and rotates relatively, it will display a linear reading stripe along the radial direction, and the scale value indicated by the linear reading stripe on the scale circle is the fabric warp density or Weft density, which can quickly and easily measure the warp and weft density of fabrics, while also ensuring high accuracy.
(Ⅱ)本发明创新设计的光栅线型,使得表示密度数的刻度随角度成近似均匀分布,读数条纹呈现简单的直线型条纹,并且集中在读数区域,可以较精确地读出织物的经纬密度,这样就较好地平衡了测量成本与精确度,是一种经济、方便同时又保证了较好精确度的新的测量方法。(II) The innovatively designed grating line type of the present invention makes the scale representing the density number approximately uniformly distributed with the angle, and the reading stripes present simple linear stripes and are concentrated in the reading area, so that the warp and weft density of the fabric can be read more accurately , which better balances the measurement cost and accuracy, and is a new measurement method that is economical, convenient and at the same time ensures better accuracy.
(Ⅲ)本发明的螺线光栅密度盘,条纹出现的角度与经纬密度近似成正比,可形成均匀刻度,并且在一定的量程内,各方向上条纹角宽度基本一致,不会出现经纬密度越大,条纹宽度越小的问题,并且读数条纹为沿矢径方向的较宽明纹,便于观测,从而提高测量的精确度;将此螺线印制或刻制为光栅后覆盖在织物上,制成“螺线光栅密度盘”。(III) In the helical grating density disc of the present invention, the angle at which stripes appear is approximately proportional to the latitude and longitude density, which can form a uniform scale, and within a certain range, the angular width of the stripes in all directions is basically the same, and there will be no increase in the latitude and longitude density. Larger, the smaller the stripe width, and the reading stripes are wider bright stripes along the radial direction, which is convenient for observation and improves the measurement accuracy; this spiral is printed or engraved as a grating and then covered on the fabric. A "spiral grating density disc" was made.
(Ⅳ)本发明的螺线光栅密度盘的量程只与极角最大与最小值有关,与光栅本身尺寸无关,因此可以根据实际测量需要任意设置量程范围来画出所需螺线光栅线;避免了传统的斜线光栅量程范围越大则光栅纵向尺寸也越大的缺点。(IV) The measuring range of the helical grating density disc of the present invention is only related to the maximum and minimum polar angles, and has nothing to do with the size of the grating itself, so the required helical grating line can be drawn by arbitrarily setting the measuring range according to the actual measurement needs; It overcomes the disadvantage that the larger the range of the traditional oblique grating is, the larger the longitudinal size of the grating is.
(Ⅴ)由于本发明的螺线光栅密度盘的光栅线为反比例螺旋曲线,各点的切线方向随极角快速变化,在其他极角方向上纱线与螺旋线交角较大,则不会形成人眼可见的莫尔条纹。即条纹只集中出现在读数位置附近,避免了传统斜线光栅密度镜中普遍存在的影响分辨读数位置的干扰条纹。(V) Since the grating line of the helical grating density disk of the present invention is an inversely proportional helical curve, the tangent direction of each point changes rapidly with the polar angle. Moiré fringes visible to the human eye. That is, the fringes only appear in the vicinity of the reading position, which avoids the interference fringes that affect the resolution of the reading position commonly existing in the traditional oblique grating densitometer.
附图说明Description of drawings
图1为本发明光栅线的示意图。FIG. 1 is a schematic diagram of a grating line of the present invention.
图2为本发明实施例1中的螺线光栅密度盘示意图。FIG. 2 is a schematic diagram of the helical grating density disk in
图3为本发明实施例2中的螺线光栅密度盘示意图。FIG. 3 is a schematic diagram of a helical grating density disk in
图4为本发明实施例3中的螺线光栅密度盘示意图。4 is a schematic diagram of a helical grating density disk in
图5为本发明实施例4中的螺线光栅密度盘测量织物密度示意图。FIG. 5 is a schematic diagram showing the density of the fabric measured by the helical grating density disc in Example 4 of the present invention.
图6为本发明实施例4中的螺线光栅密度盘测量织物密度示意图。FIG. 6 is a schematic diagram of the density of the fabric measured by the helical grating density disc in Example 4 of the present invention.
图7为本发明实施例5中的螺线光栅密度盘测量织物密度示意图。FIG. 7 is a schematic diagram of the density of the fabric measured by the helical grating density disc in Example 5 of the present invention.
图8为本发明实施例5中的螺线光栅密度盘测量织物密度示意图。FIG. 8 is a schematic diagram of the density of the fabric measured by the helical grating density disc in Example 5 of the present invention.
图9为本发明实施例6中的螺线光栅密度盘测量织物密度示意图。FIG. 9 is a schematic diagram showing the density of the fabric measured by the helical grating density disc in Example 6 of the present invention.
图10为本发明实施例7中的螺线光栅密度盘测量织物密度示意图。FIG. 10 is a schematic diagram of the density of the fabric measured by the helical grating density disc in Example 7 of the present invention.
图11为本发明实施例8中的螺线光栅密度盘测量织物密度示意图。FIG. 11 is a schematic diagram of measuring the density of the fabric by the helical grating density disc in Example 8 of the present invention.
图12为本发明实施例9中的螺线光栅密度盘测量织物密度示意图。FIG. 12 is a schematic diagram of the density of the fabric measured by the helical grating density disc in Example 9 of the present invention.
图中各标号含义:1-内圈刻度圆周,2-外圈刻度圆周,3-圆形线。The meaning of each symbol in the figure: 1- inner circle scale circumference, 2- outer circle scale circumference, 3-circular line.
具体实施方式Detailed ways
本发明提供了一种螺线光栅密度盘,包括透明基板,在透明基板上制有多条均绕同一中心原点逆时针旋转而成的反比例螺旋形的光栅线;在逆时针旋转过程中,每条光栅线的矢径长度均逐渐减小;位于最中心的光栅线的旋转角度是360度,且其他各条光栅线的旋转角度等于或小于360度;在透明基板还设有与光栅线同心的多圈刻度圆周;螺线光栅密度盘与织物重叠并相对转动时,会显示出一条沿矢径方向的直线读数条纹,该直线读数条纹在刻度圆周上所指刻度值即为织物经纱密度或纬纱密度。The invention provides a helical grating density disc, comprising a transparent substrate, on which a plurality of inversely proportional helical grating lines are formed by rotating counterclockwise around the same central origin; during the counterclockwise rotation, each The length of the vector radius of each grating line gradually decreases; the rotation angle of the grating line at the center is 360 degrees, and the rotation angle of other grating lines is equal to or less than 360 degrees; there is also a concentric grating line on the transparent substrate. When the helical grating density disc overlaps with the fabric and rotates relatively, it will display a linear reading stripe along the radial direction. The scale value indicated by the linear reading stripe on the scale circle is the fabric warp density or Weft density.
光栅线在极坐标系中满足以下方程:其中,ρ为矢径长度,即光栅线上任一点与中心原点连线的长度;n为光栅线序号,从中心原点到边缘依次取值为n=1,2,3,…;θ为极角,是矢径相对极轴(X轴)逆时针旋转转过的角度(也即矢径与极轴的夹角),θ取值在长度为2π的区间[θ1,θ2]内,θ1为最小极角,θ2=θ1+2π为最大极角;a为长度量,决定光栅线上各点矢径长度和相邻光栅线在同一极角方向上对应点矢径长度之差(即相邻光栅线在该极角方向上对应点的距离),并与极角θ共同决定螺线光栅密度盘的量程;例如当θ取值在[2π,4π]时,对第i条螺旋线,矢径长度ρ的取值范围为相邻两条光栅线的矢径长度之差为常量量程为近似为 Raster lines satisfy the following equations in polar coordinates: Among them, ρ is the length of the vector radius, that is, the length of the line connecting any point on the grating line and the central origin; n is the serial number of the grating line, which is n=1, 2, 3, ... in order from the central origin to the edge; θ is the polar angle , is the counterclockwise rotation angle of the vector radius relative to the polar axis (X axis) (that is, the angle between the vector radius and the polar axis ) . 1 is the minimum polar angle, θ 2 =θ 1 +2π is the maximum polar angle; a is the length, which determines the difference between the length of each point on the grating line and the length of the corresponding point on the adjacent grating line in the same polar angle direction (that is, the distance between the corresponding points of adjacent grating lines in the polar angle direction), and together with the polar angle θ to determine the range of the helical grating density disk; for example, when the value of θ is [2π, 4π], for the i-th Spiral line, the value range of the length ρ of the vector radius is The difference between the radial lengths of two adjacent raster lines is constant The range is approximately
本实施方式中,刻度圆周有两圈,分别为内圈刻度圆周和外圈刻度圆周,在内圈刻度圆周和外圈刻度圆周之间还设有同心的圆形线;内圈刻度圆周的半径为R,根据R值能得到内圈刻度圆周之内的光栅线的序号取值范围:内圈刻度圆周以内的光栅线的序号取值范围为n=1,2,…,nmax;序号n的光栅线的极角取值范围为θ∈[θmin,θmax];In this embodiment, the scale circle has two circles, namely the inner circle scale circle and the outer circle scale circle, and a concentric circular line is also provided between the inner circle scale circle and the outer circle scale circle; the radius of the inner circle scale circle is is R, and the value range of the serial number of the grating line within the scale circle of the inner ring can be obtained according to the R value: the value range of the serial number of the grating line within the scale circle of the inner circle is n=1,2,...,n max ; the serial number n The range of polar angle of the grating line is θ∈[θ min ,θ max ];
设序号nmax的光栅线与半径R的内圈刻度圆周交点为有可得光栅线的序号应为整数,故实际应舍去计算结果中的小数部分,取整为 Let the intersection point of the grating line with the serial number n max and the inner ring scale circle of radius R be Have Available The serial number of the raster line should be an integer, so the decimal part in the calculation result should be discarded, and the integer should be
设序号n的光栅线与半径R的内圈刻度圆周交点为有可得若θ1<γ<θ2,实际相交,则取θmin=γ,θmax=θ2;否则实际不相交,取θmin=θ1,θmax=θ2;Let the intersection of the grating line of serial number n and the circle of the inner ring scale of radius R be Have Available If θ 1 <γ<θ 2 , the actual intersection, then take θ min =γ, θ max =θ 2 ; otherwise, if they do not actually intersect, take θ min =θ 1 ,θ max =θ 2 ;
外圈刻度圆周的半径为R2,圆形线的半径为R1,外圈刻度圆周和圆形线之间为位于环带内的光栅线,根据R1和R2值能得到位于环带内的光栅线的序号取值范围:位于环带内的光栅线的序号取值范围为n=nmin,nmin+1…,nmax;序号n的光栅线的极角取值范围为θ∈[θmin,θmax];The radius of the outer ring scale circle is R 2 , the radius of the circular line is R 1 , and between the outer ring scale circle and the circular line is the grating line located in the annular band, according to the values of R 1 and R 2 , the position in the annular band can be obtained. The value range of the serial number of the grating line in the ring zone: the range of the serial number of the grating line in the annular zone is n=n min , n min +1...,n max ; the value range of the polar angle of the grating line of serial number n is θ ∈[θ min ,θ max ];
设序号nmin的光栅线与半径R1的圆形线交点为即得光栅线的序号应为整数,故实际应舍去计算结果中的小数部分,取整后再加一为 Let the intersection point of the grating line with the serial number n min and the circular line with the radius R 1 be which is have to The serial number of the raster line should be an integer, so the decimal part in the calculation result should be rounded off, and then add one to the integer.
设序号nmax的光栅线与半径R2的外圈刻度圆周交点为有得光栅线序号应为整数,故实际应舍去计算结果中的小数部分,取整为 Let the intersection point of the grating line with the serial number n max and the outer ring scale circle of radius R 2 be Have have to The serial number of the raster line should be an integer, so the decimal part of the calculation result should be discarded, and the integer should be
设序号n的光栅线与半径R1圆形线交点为有可得与半径R2的外圈刻度圆周交点为有可得显然χ<η;若θ1<η<θ2,实际与半径R1圆形线的的圆周相交,应取θmax=η,否则实际不相交,取θmax=θ2,若θ1<χ<θ2,实际与半径R2的外圈刻度圆周相交,应取θmin=χ,否则实际不相交,取θmin=θ1。Let the intersection of the grating line with the serial number n and the circular line of radius R 1 be Have Available The point of intersection with the outer ring scale circumference of radius R 2 is Have Available Obviously χ<η; if θ 1 <η<θ 2 , it actually intersects with the circumference of the circular line of radius R 1 , and θ max = η should be taken ; χ<θ 2 , which actually intersects with the scale circle of the outer ring of radius R 2 , should take θ min =χ, otherwise it does not actually intersect, take θ min =θ 1 .
各光栅线在同一极角方向上的对应点的矢径长度构成等差数列,即任意两条相邻的光栅线在同一极角方向上对应点的的间距相等,都为极角θ成反比,具有空间周期性。优选的,在本实施方式中,光栅线的自身宽度随极角变化,在任一极角方向上的宽度都相等,等于相邻光栅线在该极角方向上的对应点间距,从而黑白部分宽度相同。The length of the vector radius of the corresponding points of each grating line in the same polar angle direction constitutes an arithmetic sequence, that is, the distance between the corresponding points of any two adjacent grating lines in the same polar angle direction is equal, both are The polar angle θ is inversely proportional and has spatial periodicity. Preferably, in this embodiment, the width of the grating line itself changes with the polar angle, and the width in any polar angle direction is equal, which is equal to the corresponding point spacing of adjacent grating lines in the polar angle direction, so that the width of the black and white part is equal. same.
刻度圆周上刻度线的分布规律满足方程:其中,D为刻度值,因极角θ的平方一般远大于1,将上述刻度线分布规律公式近似为均匀刻度;刻度值为公制或英制,单位为线数/厘米或线数/英寸;The distribution law of the tick marks on the scale circle satisfies the equation: Among them, D is the scale value. Since the square of the polar angle θ is generally much larger than 1, the above-mentioned formula for the distribution law of the scale lines is approximated as Uniform scale; scale values are metric or imperial, in lines/cm or lines/inch;
a和θ的确定:Determination of a and θ:
刻度值的最小刻度值为D1,最大刻度值为D2,分别对应光栅线的最小极角θ1和最大极角θ2;其中,The minimum scale value of the scale value is D 1 , and the maximum scale value is D 2 , respectively corresponding to the minimum polar angle θ 1 and the maximum polar angle θ 2 of the grating line; among them,
螺线光栅密度盘的量程只与最小极角θ1和最大极角θ2有关,与透明基板的大小或光栅线的条数或刻度线无关,因此可以根据实际测量需要任意设置量程范围来画出所需螺线光栅线;避免了传统的斜线光栅量程范围越大则光栅纵向尺寸也越大的缺点。The range of the spiral grating density disc is only related to the minimum polar angle θ 1 and the maximum polar angle θ 2 , and has nothing to do with the size of the transparent substrate or the number of grating lines or scale lines, so the measurement range can be arbitrarily set according to the actual measurement. The required helical grating line is obtained; the disadvantage of the traditional oblique grating that the larger the range is, the larger the longitudinal size of the grating is.
刻度圆周的分布规律方程的公式推导如下:The distribution law equation of the scale circle The formula is derived as follows:
当θ=θ0为任一固定值时,序号为n的光栅线在极角θ0方向上对应点的矢径长度为即该点极坐标为相邻两条光栅线的矢径长度之差为常量 When θ=θ 0 is any fixed value, the radial vector length of the corresponding point of the grating line with serial number n in the direction of polar angle θ 0 is That is, the polar coordinates of the point are The difference between the radial lengths of two adjacent raster lines is constant
如图1所示,曲线L1为光栅线,直线L2为极角θ0方向的矢径,直线L3为各光栅线在极角θ0方向的对应点处的切线,直线L4为与各切线垂直的法线方向的矢径;As shown in Figure 1, the curve L1 is the grating line, the straight line L2 is the vector radius in the direction of the polar angle θ 0 , and the straight line L3 is the corresponding point of each grating line in the direction of the polar angle θ 0 The tangent at , the straight line L4 is the vector radius of the normal direction perpendicular to each tangent;
直线L4与极轴(X轴)夹角为φ,直线L4与直线L2夹角为φ-θ0,直线L3与直线L2的夹角为α; The angle between the line L4 and the polar axis (X axis) is φ, the angle between the line L4 and the line L2 is φ-θ 0 , and the angle between the line L3 and the line L2 is α;
光栅线上一点处的切线方程为ρcos(θ-φ)=nd,其中,n为切线序号,也为光栅线序号;A point on the raster line The tangent equation at is ρcos(θ-φ)=nd, where n is the serial number of the tangent, which is also the serial number of the grating line;
切线均互相平行且等间距,切线斜率均为该斜率与n值无关;d为相邻两条切线之间的距离,螺线光栅密度盘与织物相对转动,直至光栅线的切线与织物的纱线重合时,得到纱线密度 The tangents are all parallel and equally spaced, and the slopes of the tangents are The slope is independent of the value of n; d is the distance between two adjacent tangents, The helical grating density disc rotates relative to the fabric until the tangent of the grating line coincides with the yarn of the fabric to obtain the yarn density
当织物的经纱(或纬纱)与光栅线在某一极角θ0方向的对应点处的切线平行,且纱线间距与切线间距相近时,根据形成莫尔条纹的阴影遮光原理或空间拍频原理,在该极角方向附近出现莫尔条纹,条纹的空间频率等于纱线空间频率与切线空间频率之差;When the warp (or weft) of the fabric is parallel to the tangent of the grating line at the corresponding point in the direction of a certain polar angle θ 0 , and the yarn spacing is similar to the tangent spacing, according to the shadow shading principle or spatial beat frequency that forms moire fringes According to the principle, moire fringes appear near the polar angle direction, and the spatial frequency of the fringes is equal to the difference between the spatial frequency of the yarn and the spatial frequency of the tangent;
当织物经纱间距等于光栅线在极角θ0方向的对应点处的的切线间距时,则莫尔条纹空间频率为零,即莫尔条纹间距无穷大;则此处出现一条沿θ0方向无限延伸的较宽的明条纹,即直线读数条纹;直线读数条纹在刻度圆周上所指刻度值即为织物经纱或纬纱密度;由于光栅线为反比例螺旋曲线,各点的切线方向随极角快速变化,在其他极角方向上纱线与螺旋线交角较大,则不会形成人眼可见的莫尔条纹;直线读数条纹只集中出现在读数位置附近,避免了传统斜线光栅中普遍存在的影响分辨读数位置的干扰条纹;When the warp pitch of the fabric is equal to the tangent pitch of the grating line at the corresponding point in the polar angle θ 0 direction, the spatial frequency of the moiré fringes is zero, that is, the moiré fringe pitch is infinite; then there is a line extending infinitely along the θ 0 direction. The wider bright stripes, that is, the linear reading stripes; the linear reading stripes refer to the scale value on the scale circle That is, the density of the warp or weft of the fabric; since the grating line is an inversely proportional helical curve, the tangent direction of each point changes rapidly with the polar angle, and the intersection angle between the yarn and the helix in other polar angles is large, and it will not be visible to the human eye. Moiré fringes; linear reading fringes only appear near the reading position, avoiding the interference fringes that affect the resolution of the reading position commonly found in traditional oblique gratings;
具体的,在θ0方向出现直线读数条纹的原理:当织物经纱间距等于θ0方向的光栅线的切线间距时,与织物重叠的螺线光栅密度盘显示出一条沿矢径方向的直线读数条纹,该直线读数条纹在刻度圆周上所指刻度值为织物经纱密度其中,经纱间距为 Specifically, the principle of linear reading stripes appearing in the θ 0 direction: when the warp distance of the fabric is equal to the tangent spacing of the grating lines in the θ 0 direction, the helical grating density disc overlapping the fabric shows a linear reading stripe along the radial direction. , the linear reading stripes on the scale circle refer to the scale value of the fabric warp density Among them, the warp distance is
设初始经纱方程为ρcosθ=nd,n=1,2,…,即经纱初始平行于y轴,与θ=2π方向的矢径垂直,将织物沿逆时针方向转过φ角度,经纱方程变为ρcos(θ-φ)=nd,则此时经纱恰与光栅线θ=θ0方向对应点处的切线重合,根据光栅透过率的空间频率理论可知,经纱视为直线光栅,其透过率的空间频率矢量沿极角φ方向,大小为则沿极角θ0方向的投影分量为光栅线沿极角θ0方向周期为透过率的空间频率经纱和光栅线在极角θ0方向重叠后总透过率的空间频率大小为K=|K1-K2|=0,则空间周期,即莫尔条纹间距趋于无穷大,因而在此θ0方向上,形成的莫尔条纹间距将趋于无穷大;而在此θ0方向附近,设偏离微小角度δ,|δ|<5°,相应空间频率大小变为:Let the initial warp equation be ρcosθ=nd, n=1, 2,..., that is, the warp is initially parallel to the y-axis and perpendicular to the radial vector in the direction of θ=2π, and the fabric is rotated counterclockwise through the angle φ, and the warp equation becomes ρcos(θ-φ)=nd, then the warp is just the corresponding point in the direction of the grating line θ=θ 0 The tangents at the position coincide, according to the spatial frequency theory of grating transmittance, the warp is regarded as a linear grating, and the spatial frequency vector of its transmittance Along the polar angle φ direction, the magnitude is but The projected component along the polar angle θ 0 direction is The period of the grating line along the polar angle θ 0 is Spatial frequency of transmittance The spatial frequency of the total transmittance after the warp yarn and the grating line overlap in the polar angle θ 0 direction is K=|K 1 -K 2 |=0, then the spatial period, that is, the Moire fringe spacing tends to infinity, so in the θ 0 direction, the formed Moiré fringe spacing will tend to be infinite; and in the vicinity of this θ 0 direction, if the deviation is a small angle δ, |δ|<5°, the corresponding spatial frequency becomes :
K′1与K′2相差很小,因此总透过率空间频率K’很小,出现“拍”现象,周期很大,即条纹间距亦很大,因此在θ0方向附近有限距离内将只观察到一条较宽明条纹,即直线读数条纹;The difference between K' 1 and K' 2 is very small, so the spatial frequency K' of the total transmittance is very small, and a "beat" phenomenon occurs, and the period is very large, that is, the fringe spacing is also very large, so only a wide bright fringe, that is, a straight reading fringe, will be observed within a limited distance near the θ 0 direction;
或者解释为经纱与光栅线的交点中,那些间距较小的交点连线形成明条纹,在θ0处经纱与光栅线相切,因此在θ0附近,经纱与光栅线的交点距离切点较远,而相邻切点间距较小,各切点连线形成莫尔条纹;该条纹对应角度θ0即可代表示经纱密度;经纱密度0近似与极角θ0成正比;因此把D作为读数在刻度圆周上标注,将形成近似呈均匀分布的刻度,各角度方向上出现的读数条纹角宽度亦基本一致;类似的也可用对应条纹代表纬纱密度。Or it can be explained that among the intersections of warp and grating lines, those intersections with smaller distances form bright fringes, and at θ 0 the warp is tangent to the grating line, so near θ 0 , the intersection of the warp and the grating line is farther from the tangent point. The distance between adjacent tangent points is small, and each tangent point is connected to form Moiré fringes; the corresponding angle θ 0 of the fringes can represent the warp density; the
极角公式推导:若根据近似结果经纱密度标定刻度会有微小误差,相对误差约为绝对误差约为例如当θ0取值在[2π,4π]区间内时,相对误差范围约0.32%至1.27%,若设a=0.1π厘米,则量程近似为线/厘米,绝对误差约为0.13至0.25线/厘米,θ0取值越大,误差越小。The derivation of the polar angle formula: if the warp density is based on the approximate result There will be a small error in the calibration scale, and the relative error is about The absolute error is about For example, when the value of θ 0 is within the interval of [2π, 4π], the relative error range is about 0.32% to 1.27%. If a=0.1π cm, the range is approximately Line/cm, the absolute error is about 0.13 to 0.25 line/cm, the larger the value of θ 0 , the smaller the error.
标定刻度时可根据实际量程标定刻度;When calibrating the scale, it can be based on the actual range calibration scale;
即量程下限为上限 That is, the lower limit of the range is upper limit
可算出θ1为与下限D1对应的最小极角,θ1+2π=θ2为与上限D2对应的最大极角;根据此a和θ1能画出光栅线。can be calculated θ 1 is the minimum polar angle corresponding to the lower limit D 1 , and θ 1 +2π=θ 2 is the maximum polar angle corresponding to the upper limit D 2 ; according to this a and θ 1 can draw grating lines.
然后根据在极角θ0方向标注刻度读数D即可不产生此误差。因为近似值与精确值间误差很小,所以精确标定刻度并不影响刻度基本呈均匀分布,但有利于得到更精确的测量结果。then according to This error can be avoided by marking the scale reading D in the polar angle θ 0 direction. Because the error between the approximate value and the exact value is very small, the accurate calibration of the scale does not affect the basic uniform distribution of the scale, but it is beneficial to obtain more accurate measurement results.
本发明还提供一种织物经纬密度的测量方法,该测量方法采用上述螺线光栅密度盘进行测量,该测量方法的步骤如下:The present invention also provides a method for measuring the warp and weft density of fabrics. The measuring method adopts the above-mentioned helical grating density disc to measure, and the steps of the measuring method are as follows:
步骤一:将所述螺线光栅密度盘覆盖在织物上,初始在近似垂直于织物经纱(或纬纱)方向附近会出现多条弯曲的明暗相间的条纹;Step 1: Cover the helical grating density disk on the fabric, and initially there will be a plurality of curved light and dark stripes near the direction approximately perpendicular to the warp (or weft) of the fabric;
步骤二:然后转动所述螺线光栅密度盘,使弯曲的条纹数逐渐减少,直至最终只显示为一条沿矢径方向的较宽明条纹,即直线读数条纹,该直线读数条纹在对应刻度圆周上所指刻度值即为织物经纱密度或纬纱密度。Step 2: Then turn the helical grating density disk to gradually reduce the number of curved stripes until finally only a wider bright stripe along the radial direction is displayed, that is, a straight reading stripe, which is on the corresponding scale circle. The scale value indicated above is the fabric warp density or weft density.
织物的纱线间距与经纬密度成反比。常见织物经纬密度范围约为10~120线/cm,即纱线间距在1/10~1/120cm;本实施方式中的螺线光栅密度盘在测量过程中显示的直线读数条纹长度大于1cm,便于观察读数。The yarn spacing of the fabric is inversely proportional to the warp and weft density. The warp and weft density range of common fabrics is about 10 to 120 threads/cm, that is, the yarn spacing is 1/10 to 1/120 cm. Easy to observe readings.
本实施方式是通过MATLAB软件画出螺线光栅密度盘和织物纱线,再通过螺线光栅密度盘和织物纱线之间的相对转动进行如下实施例中的测量。In this embodiment, the helical grating density disc and the fabric yarn are drawn by MATLAB software, and then the measurement in the following embodiment is performed through the relative rotation between the helical grating density disc and the fabric yarn.
遵从上述技术方案,以下给出本发明的具体实施例,需要说明的是本发明并不局限于以下具体实施例,凡在本申请技术方案基础上做的等同变换均落入本发明的保护范围。下面结合实施例对本发明做进一步详细说明。Following the above technical solutions, specific embodiments of the present invention are given below. It should be noted that the present invention is not limited to the following specific embodiments, and all equivalent transformations made on the basis of the technical solutions of the present application all fall into the protection scope of the present invention. . The present invention will be described in further detail below in conjunction with the embodiments.
实施例1:Example 1:
如图2所示,本发明实施例1提供一种量程为10~40线/厘米的螺线光栅密度盘,设计量程为10~40线/厘米,图形大小13*13(厘米);As shown in FIG. 2,
内圈光栅线量程10~25,为使测量值恰好在量程边界附近时便于观测形成的莫尔条纹,实际画图时量程下限和上限分别扩展0.5,即实际取D1=9.5,D2=25.5,则 The inner ring grating line has a range of 10 to 25. In order to make the measurement value just near the range boundary to facilitate the observation of the moire fringes formed, the lower and upper limits of the range are expanded by 0.5 respectively during the actual drawing, that is, D 1 =9.5, D 2 =25.5 ,but
外圈光栅线量程25~40,为使测量值恰好在量程边界附近时便于观测形成的莫尔条纹,实际画图时量程下限和上限分别扩展0.5,即实际取D1=24.5,D2=40.5,则 The outer ring grating line has a range of 25 to 40. In order to make the measurement value just near the range boundary to facilitate the observation of the moire fringes formed, the lower limit and upper limit of the range are expanded by 0.5 respectively during the actual drawing, that is, D 1 =24.5, D 2 =40.5 ,but
内圈光栅线画在半径为R=3.5厘米的内圈刻度圆周内,外圈光栅线画在半径R2=6厘米的外圈刻度圆周和半径R1=4厘米的圆形线之间的环带内。The grating line of the inner ring is drawn within the scale circle of the inner ring with a radius of R = 3.5 cm, and the grating line of the outer ring is drawn between the scale circle of the outer ring with a radius of R 2 = 6 cm and a circular line with a radius of R 1 = 4 cm. inside the ring.
采用本实施例1中的螺线光栅密度盘测量织物密度的测量数据如下表1至表3所示。The measurement data for measuring the fabric density using the helical grating density disc in this Example 1 are shown in Tables 1 to 3 below.
实施例2:Example 2:
如图3所示,本发明实施例2提供一种量程为40~80线/厘米的螺线光栅密度盘,设计量程为40~80线/厘米,图形大小13*13(厘米);As shown in FIG. 3,
内圈光栅线量程40~60,为使测量值恰好在量程边界附近时便于观测形成的莫尔条纹,实际画图时量程下限和上限分别扩展0.5,即实际取D1=39.5,D2=60.5,则 The inner ring grating line has a range of 40 to 60. In order to make the measurement value just near the range boundary to facilitate the observation of the moire fringes formed, the lower limit and upper limit of the range are expanded by 0.5 respectively during the actual drawing, that is, D 1 =39.5, D 2 =60.5 ,but
外圈光栅线量程60~80,为使测量值恰好在量程边界附近时便于观测形成的莫尔条纹,实际画图时量程下限和上限分别扩展0.5,即实际取D1=24.5,D2=40.5,则 The outer ring grating line has a range of 60 to 80. In order to make the measurement value just near the range boundary to facilitate the observation of the moire fringes formed, the lower limit and upper limit of the range are expanded by 0.5 respectively during the actual drawing, that is, D 1 =24.5, D 2 =40.5 ,but
内圈光栅线画在半径为R=3.5厘米的内圈刻度圆周内,外圈光栅线画在半径R2=6厘米的外圈刻度圆周和半径R1=4厘米的圆形线之间的环带内。The grating line of the inner ring is drawn within the scale circle of the inner ring with a radius of R = 3.5 cm, and the grating line of the outer ring is drawn between the scale circle of the outer ring with a radius of R 2 = 6 cm and a circular line with a radius of R 1 = 4 cm. inside the ring.
实施例3:Example 3:
如图4所示,本发明实施例3提供一种量程为80~120线/厘米的螺线光栅密度盘,设计量程为80~120线/厘米,图形大小13*13(厘米);As shown in FIG. 4 ,
内圈光栅线量程80~100,为使测量值恰好在量程边界附近时便于观测形成的莫尔条纹,实际画图时量程下限和上限分别扩展0.5,即实际取D1=79.5,D2=100.5,则 The inner ring grating line has a range of 80 to 100. In order to make the measurement value just near the range boundary to facilitate the observation of the moire fringes formed, the lower limit and upper limit of the range are expanded by 0.5 respectively during the actual drawing, that is, D 1 =79.5, D 2 =100.5 ,but
外圈光栅线量程100~120,为使测量值恰好在量程边界附近时便于观测形成的莫尔条纹,实际画图时量程下限和上限分别扩展0.5,即实际取D1=99.5,D2=120.5,则 The outer ring grating line has a range of 100 to 120. In order to make the measurement value just near the range boundary to facilitate the observation of the moire fringes formed, the lower limit and upper limit of the range are expanded by 0.5 respectively during the actual drawing, that is, D 1 =99.5, D 2 =120.5 ,but
内圈光栅线画在半径为R=3.5厘米的内圈刻度圆周内,外圈光栅线画在半径R2=6厘米的外圈刻度圆周和半径R1=4厘米的圆形线之间的环带内。The grating line of the inner ring is drawn within the scale circle of the inner ring with a radius of R = 3.5 cm, and the grating line of the outer ring is drawn between the scale circle of the outer ring with a radius of R 2 = 6 cm and a circular line with a radius of R 1 = 4 cm. inside the ring.
实施例4:Example 4:
如图5和图6所示,本发明实施例提供一种采用实施例1中的螺线光栅密度盘测量织物密度的方法,如图5所示:平行的竖线代表织物的经纱,开始平行于y轴方向,纱线间距d=1/18厘米,对应经纱密度为D=18线/厘米,现在显示为多条弯曲花纹。如图6所示:使织物与螺线光栅密度盘发生相对转动,最终在刻度18处显示仅有一条沿矢径方向的较宽明条纹,即直线读数条纹所指示的读数为18线/厘米。As shown in Fig. 5 and Fig. 6, an embodiment of the present invention provides a method for measuring the density of a fabric by using the spiral grating density disc in
实施例5:Example 5:
如图7和图8所示,本发明实施例提供一种采用实施例1中的螺线光栅密度盘测量织物密度的方法,如图7所示:平行的直线线代表织物的经(纬)纱,开始平行于y轴方向,纱线间距d=1/36厘米,对应密度为D=36线/厘米。如图8所示,织物与螺线光栅密度盘发生相对转动后在刻度36处显示仅有一条较宽明纹,即直线读数条纹所指示的读数为36线/厘米。As shown in FIG. 7 and FIG. 8 , an embodiment of the present invention provides a method for measuring fabric density by using the spiral grating density disc in
实施例6:Example 6:
如图9所示,本发明实施例提供一种采用实施例2中的螺线光栅密度盘测量织物密度的方法,如图9所示:织物与螺线光栅密度盘发生相对转动后在刻度45处显示仅有一条较宽明纹,即直线读数条纹所指示的读数为45线/厘米。As shown in FIG. 9 , an embodiment of the present invention provides a method for measuring fabric density by using the helical grating density disc in
实施例7:Example 7:
如图10所示,本发明实施例提供一种采用实施例2中的螺线光栅密度盘测量织物密度的方法,如图10所示:织物与螺线光栅密度盘发生相对转动后在刻度75处显示仅有一条较宽明纹,即直线读数条纹所指示的读数为75线/厘米。As shown in FIG. 10 , an embodiment of the present invention provides a method for measuring fabric density by using the helical grating density disc in
实施例8:Example 8:
如图11所示,本发明实施例提供一种采用实施例3中的螺线光栅密度盘测量织物密度的方法,如图11所示:织物与螺线光栅密度盘发生相对转动后在刻度95处显示仅有一条较宽明纹,即直线读数条纹所指示的读数为95线/厘米。As shown in FIG. 11 , an embodiment of the present invention provides a method for measuring fabric density by using the helical grating density disc in
实施例9:Example 9:
如图12所示,本发明实施例提供一种采用实施例3中的螺线光栅密度盘测量织物密度的方法,如图12所示:织物与螺线光栅密度盘发生相对转动后在刻度110处显示仅有一条较宽明纹,即直线读数条纹所指示的读数为110线/厘米。As shown in FIG. 12 , an embodiment of the present invention provides a method for measuring fabric density by using the helical grating density disc in
通过实施例1至实施例9可以看出,本发明的螺线光栅密度盘可以快速方便并较精确地测出平纹织物的经纬密度。It can be seen from Examples 1 to 9 that the helical grating density disc of the present invention can quickly, conveniently and accurately measure the warp and weft density of plain weave fabrics.
对比例1:Comparative Example 1:
本对比例采用传统斜线光栅密度镜测量织物密度,测量结果如表1至表3所示。本对比例采用的斜线光栅密度镜是常规的仪器。In this comparative example, the traditional diagonal grating densitometer is used to measure the fabric density, and the measurement results are shown in Tables 1 to 3. The oblique grating density mirror used in this comparative example is a conventional instrument.
对比例2:Comparative Example 2:
本对比例采用读数显微镜测量织物密度,测量结果如表1至表3所示。本对比例采用的读数显微镜也是常规的仪器。In this comparative example, the density of the fabric was measured by a reading microscope, and the measurement results are shown in Tables 1 to 3. The reading microscope used in this comparative example is also a conventional instrument.
表1为实施例1、对比例1和对比例2测量织物密度原始数据(单位:线/厘米)Table 1 is the raw data of fabric density measured in Example 1, Comparative Example 1 and Comparative Example 2 (unit: thread/cm)
表2为实施例1、对比例1和对比例2测量织物密度的不确定度分析数据Table 2 is the uncertainty analysis data for the measurement of fabric density in Example 1, Comparative Example 1 and Comparative Example 2
表3为实施例1、对比例1和对比例2测量织物密度的测量结果比较(单位:线/厘米)Table 3 is a comparison of the measurement results of the fabric density measured in Example 1, Comparative Example 1 and Comparative Example 2 (unit: thread/cm)
从上述表1至表3可以看出,本发明密度盘测量结果接近读数显微镜,虽然读数显微镜测量精确度较高,但配置仪器或人工成本很高,测量速度也较慢。本发明密度盘测量的精确度高于传统的密度镜,主要原因是传统密度镜显示的莫尔条纹分布为分散的反比例曲线,各处都会出现莫尔条纹,且不同位置条纹大小不均匀,刻度线随读数值增大越来越密集,呈现非均匀刻度,因此读数位置不易对准。而密度盘条纹呈现沿矢径方向的直线型条纹,不同位置条纹长度相同且角宽度差异很小,且出现的条纹集中分布在读数位置附近,刻度线随读数变化基本成均匀刻度,因此较易对准读数位置,从而提高了测量结果的精确度。As can be seen from the above Tables 1 to 3, the measurement results of the density disc of the present invention are close to that of the reading microscope. Although the measurement accuracy of the reading microscope is high, the cost of configuring instruments or labor is high, and the measurement speed is also relatively slow. The measurement accuracy of the density disc of the present invention is higher than that of the traditional density mirror. The main reason is that the Moiré fringe distribution displayed by the traditional density mirror is a scattered inverse proportional curve. The lines become denser and denser as the reading value increases, showing a non-uniform scale, so the reading position is not easy to align. The density disc stripes are linear stripes along the radial direction. The stripes at different positions have the same length and little difference in angular width, and the stripes appear concentrated near the reading position. Align the reading position, thereby improving the accuracy of the measurement results.
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Citations (7)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US4116566A (en) * | 1975-11-12 | 1978-09-26 | Erwin Sick Gesellschaft Mit Beschrankter Haftung Optik-Elektronik | Line scanning device for detecting defects in webs of material |
CN86103771A (en) * | 1986-06-04 | 1987-01-31 | 北京工业学院 | Constitute little deviation meter with specific not equidistant screen |
CN87102127A (en) * | 1987-03-12 | 1988-09-21 | 周宇怀 | A kind of protractor |
CN2240711Y (en) * | 1995-05-12 | 1996-11-20 | 潘志刚 | Oblique line raster density instrument |
CN203642844U (en) * | 2014-01-18 | 2014-06-11 | 中国石油大学(华东) | Rock core geologic body measuring apparatus |
CN104504197A (en) * | 2014-12-21 | 2015-04-08 | 浙江省计量科学研究院 | Archimedes spiral planar thread measurement model and eccentric parameter correction method |
CN109594319A (en) * | 2019-01-07 | 2019-04-09 | 东华大学 | A kind of pck count intelligent detection device and method |
-
2019
- 2019-05-31 CN CN201910470968.3A patent/CN110241602B/en not_active Expired - Fee Related
Patent Citations (7)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US4116566A (en) * | 1975-11-12 | 1978-09-26 | Erwin Sick Gesellschaft Mit Beschrankter Haftung Optik-Elektronik | Line scanning device for detecting defects in webs of material |
CN86103771A (en) * | 1986-06-04 | 1987-01-31 | 北京工业学院 | Constitute little deviation meter with specific not equidistant screen |
CN87102127A (en) * | 1987-03-12 | 1988-09-21 | 周宇怀 | A kind of protractor |
CN2240711Y (en) * | 1995-05-12 | 1996-11-20 | 潘志刚 | Oblique line raster density instrument |
CN203642844U (en) * | 2014-01-18 | 2014-06-11 | 中国石油大学(华东) | Rock core geologic body measuring apparatus |
CN104504197A (en) * | 2014-12-21 | 2015-04-08 | 浙江省计量科学研究院 | Archimedes spiral planar thread measurement model and eccentric parameter correction method |
CN109594319A (en) * | 2019-01-07 | 2019-04-09 | 东华大学 | A kind of pck count intelligent detection device and method |
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