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There has also been a development in free hand machine embroidery, new machines have been designed that allow for the user to create free-motion embroidery which has its place in textile arts, quilting, dressmaking, home furnishings and more. Users can use the embroidery software to digitize the digital embroidery designs.
Quilting templates/patterns come in many varieties and are generally considered the basis of the structure of the quilt, like a blueprint for a house. Bias binding or bias tape can be made from strips of quilt fabric or purchased as quilt binding. It is used in the last stage of making a quilt, and is a method of covering the edges of the quilt.
A free motion equation need not exist in general. It can be defined if and only if a configuration bundle Q → R {\displaystyle Q\to \mathbb {R} } of a mechanical system is a toroidal cylinder T m × R k {\displaystyle T^{m}\times \mathbb {R} ^{k}} .
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Bridle rolls are used to increase or decrease the strip tension in a processing line or rolling mill. Sketch 7 shows two, three and four roll bridles indicating the variables. The bridle rolls normally come in a set of two, three, or four rolls of equal diameter, with each roll individually powered by an electric motor/generator. [18]
Whole-cloth quilt, 18th century, Netherlands.Textile made in India. In Europe, quilting appears to have been introduced by Crusaders in the 12th century (Colby 1971) in the form of the aketon or gambeson, a quilted garment worn under armour which later developed into the doublet, which remained an essential part of fashionable men's clothing for 300 years until the early 1600s.
In these, one end of the bimetallic strip is mechanically fixed and attached to an electrical power source, while the other (moving) end carries an electrical contact. In adjustable thermostats another contact is positioned with a regulating knob or lever. The position so set controls the regulated temperature, called the set point.
For continuous bodies these laws are called Euler's laws of motion. [ 7 ] The total body force applied to a continuous body with mass m , mass density ρ , and volume V , is the volume integral integrated over the volume of the body: