force polygon construction - meaning and definition. What is force polygon construction
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What (who) is force polygon construction - definition

ADDITION OF VECTORS
Parallelogram of forces; Polygon of force
  • Figure 2: Parallelogram of velocity

Midpoint polygon         
  • The [[Varignon parallelogram]]
POLYGON WHOSE VERTICES ARE THE MIDPOINTS OF THE EDGES OF ANOTHER POLYGON
Midpoint Polygon; Kasner polygon; Mid-point polygon; Kasner descendant; Kasner descendent
In geometry, the midpoint polygon of a polygon is the polygon whose vertices are the midpoints of the edges of . It is sometimes called the Kasner polygon after Edward Kasner, who termed it the inscribed polygon "for brevity".
Skew polygon         
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  • A uniform ''n''-gonal [[antiprism]] has a 2''n''-sided regular skew polygon defined along its side edges.
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POLYGON WHOSE VERTICES DO NOT LIE IN A PLANE
Regular skew polygon; Space polygon; Saddle polygon; Regular skew pentagon; Regular skew decagon; Regular skew dodecagon
In geometry, a skew polygon is a polygon whose vertices are not all coplanar. Skew polygons must have at least four vertices.
Tangential polygon         
CONVEX POLYGON THAT CONTAINS AN INSCRIBED CIRCLE
Circumscribed polygon
In Euclidean geometry, a tangential polygon, also known as a circumscribed polygon, is a convex polygon that contains an inscribed circle (also called an incircle). This is a circle that is tangent to each of the polygon's sides.

Wikipedia

Parallelogram of force

The parallelogram of forces is a method for solving (or visualizing) the results of applying two forces to an object.

When more than two forces are involved, the geometry is no longer parallelogrammatic, but the same principles apply. Forces, being vectors are observed to obey the laws of vector addition, and so the overall (resultant) force due to the application of a number of forces can be found geometrically by drawing vector arrows for each force. For example, see Figure 1. This construction has the same result as moving F2 so its tail coincides with the head of F1, and taking the net force as the vector joining the tail of F1 to the head of F2. This procedure can be repeated to add F3 to the resultant F1 + F2, and so forth.