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{"id":314,"date":"2024-10-04T02:07:57","date_gmt":"2024-10-03T19:07:57","guid":{"rendered":"http:\/\/www.tneutron.net\/mesin\/?p=314"},"modified":"2024-10-01T10:58:27","modified_gmt":"2024-10-01T03:58:27","slug":"add-style-by-way-painting","status":"publish","type":"post","link":"https:\/\/www.tneutron.net\/mesin\/add-style-by-way-painting\/","title":{"rendered":"Add Style By Way Painting"},"content":{"rendered":"

If there are two forces that have captured the same point a different direction with the direction of the force makes an angle \u03b1 the resultant number can be calculated by the following equation:<\/span><\/p>\n

\"image\"<\/a><\/p>\n

Figure 2.23 Two styles with different directions<\/span><\/p>\n

\"image\"<\/a><\/p>\n

For \u03b1 = 90 \u00b0<\/sup> then Cos \u03b1 = 0 or apply the formula of Pythagoras, namely:<\/span><\/p>\n

\"image\"<\/a><\/p>\n

Description :<\/span>
\n o P and Q = component force<\/span>
\n o \u03b1 = angle of the wedge between the two styles<\/span>
\n o R = Resultant<\/span><\/p>\n

Compiling Style Located In The Flat Field<\/strong><\/span>
\n If there are two forces that have a different fishing spot and is located on a flat, then to determine the capture point style can be implemented in two ways:<\/span>
\n o by way of painting.<\/span>
\n o by way of analysis \/ count<\/span>
\n Example: Two forces each has a capture point at point A and point B with the distance AB = 60 cm, a large force P = 8 N and the direction of his style left under an angle of 120 \u00b0<\/sup> to the horizontal line, Style Q = 2 \u221a3 N with direction of the force perpendicular to the bottom, see the following picture:<\/span><\/p>\n

\"image\"<\/a><\/p>\n

Figure 2.26 Two different styles to capture titk<\/span><\/p>\n

Of both style over specified:<\/span>
\n – The magnitude of the resultant;<\/span>
\n – Directions resultant;<\/span>
\n – Point the resultant catch<\/span><\/p>\n

Completion See the following picture:<\/span>
\n To determine the point of capture, the direction and magnitude of the resultant force can be done by way of painting is as follows:<\/span>
\n – Copy the above questions with a scale of 2 N # 1cm style and length scales of 1: 10.<\/span>
\n – Extend the line of force P and Q upwards to meet at a point C.<\/span>
\n – Move the force P and Q to point C.<\/span>
\n – Create parallelogram through force P and Q are.<\/span>
\n – Create diagonally through point C to obtain the magnitude of the resultant R.<\/span>
\n – Extend the working line style R to cut the line AB at point D, and point D is the point of the resultant catch.<\/span>
\n – Move resultant from point C to point D capture.<\/span> Then obtained: the point of capture, the direction and magnitude of the resultant force as shown in the following figure.<\/span><\/p>\n

\"image\"<\/a><\/p>\n

Figure 2.27 Moving style<\/span><\/p>\n

\"image\"<\/a><\/p>\n

2:28 Figure Painting style<\/span><\/p>\n","protected":false},"excerpt":{"rendered":"

If there are two forces that have captured the same point a different direction with the direction of the force makes an angle \u03b1 the resultant number can be calculated by the following equation: Figure 2.23 Two styles with different directions For \u03b1 = 90 \u00b0 then Cos \u03b1 = 0 or apply the formula …<\/p>\n","protected":false},"author":1,"featured_media":0,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[1406],"tags":[263,259,260,261,256,257,262,254,255,258],"class_list":["post-314","post","type-post","status-publish","format-standard","hentry","category-english","tag-easy-way-painting","tag-milky-way-painting","tag-one-way-painting-erie-pa","tag-one-way-painting-lynn-ma","tag-painting-my-way","tag-right-way-painting","tag-rite-way-painting","tag-way-painting","tag-way-painting-wall","tag-wright-way-painting"],"_links":{"self":[{"href":"https:\/\/www.tneutron.net\/mesin\/wp-json\/wp\/v2\/posts\/314","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.tneutron.net\/mesin\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/www.tneutron.net\/mesin\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/www.tneutron.net\/mesin\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/www.tneutron.net\/mesin\/wp-json\/wp\/v2\/comments?post=314"}],"version-history":[{"count":1,"href":"https:\/\/www.tneutron.net\/mesin\/wp-json\/wp\/v2\/posts\/314\/revisions"}],"predecessor-version":[{"id":3149,"href":"https:\/\/www.tneutron.net\/mesin\/wp-json\/wp\/v2\/posts\/314\/revisions\/3149"}],"wp:attachment":[{"href":"https:\/\/www.tneutron.net\/mesin\/wp-json\/wp\/v2\/media?parent=314"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.tneutron.net\/mesin\/wp-json\/wp\/v2\/categories?post=314"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.tneutron.net\/mesin\/wp-json\/wp\/v2\/tags?post=314"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}