{"id":213,"date":"2022-02-23T03:53:05","date_gmt":"2022-02-23T03:53:05","guid":{"rendered":"https:\/\/smallsteamengines.com\/?page_id=213"},"modified":"2022-02-23T04:36:21","modified_gmt":"2022-02-23T04:36:21","slug":"why-compressed-air","status":"publish","type":"page","link":"https:\/\/smallsteamengines.com\/index.php\/why-compressed-air\/","title":{"rendered":"Why compressed Air?"},"content":{"rendered":"\n<p>Example of content page appearance.<\/p>\n\n\n\n<p>constant force, acting on a particle of mass m, will produce a constant acceleration a. Let us choose the x-axis to be in the common direction of F and a. What is the work done by this force on the particle in causing a displacement x? We have, for constant acceleration, the relations a = ( V &#8211; v ) \/ t and x = \u00bd ( V + v ) t. Here v is the particle&#8217;s speed at t = 0 and V is its speed at time t. The the work done is W = F x = m a x = m ( ( V &#8211; v ) \/ t ) ( \u00bd ( V + v ) ) t = \u00bd m V\u00b2 &#8211; \u00bd m v\u00b2. We call one-half the product of the mass of a body and the square of its speed the kinetic energy of the body. If we represent kinetic energy by the symbol K, then K = \u00bd m v\u00b2. We may then state the above equation in this way: The work done by the resultant force acting on a particle is equal to the change in the kinetic energy of the particle.<\/p>\n\n\n\n<div class=\"wp-block-image\"><figure class=\"aligncenter size-full\"><img loading=\"lazy\" decoding=\"async\" width=\"300\" height=\"276\" src=\"https:\/\/smallsteamengines.com\/wp-content\/uploads\/2022\/02\/6aee063384a932ec5a8c3e22f2dc62be.jpg\" alt=\"Inventors during this age filed numerous patents for engine designs. From these, scale models can be built to demonstrate their ability to function.\" class=\"wp-image-222\"\/><figcaption>Inventors file thousands of patents for engine designs.<\/figcaption><\/figure><\/div>\n","protected":false},"excerpt":{"rendered":"<p>Example of content page appearance. constant force, acting on a particle of mass m, will produce a&#8230;<\/p>\n","protected":false},"author":1,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"footnotes":""},"class_list":["post-213","page","type-page","status-publish","hentry"],"_links":{"self":[{"href":"https:\/\/smallsteamengines.com\/index.php\/wp-json\/wp\/v2\/pages\/213","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/smallsteamengines.com\/index.php\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/smallsteamengines.com\/index.php\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/smallsteamengines.com\/index.php\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/smallsteamengines.com\/index.php\/wp-json\/wp\/v2\/comments?post=213"}],"version-history":[{"count":4,"href":"https:\/\/smallsteamengines.com\/index.php\/wp-json\/wp\/v2\/pages\/213\/revisions"}],"predecessor-version":[{"id":228,"href":"https:\/\/smallsteamengines.com\/index.php\/wp-json\/wp\/v2\/pages\/213\/revisions\/228"}],"wp:attachment":[{"href":"https:\/\/smallsteamengines.com\/index.php\/wp-json\/wp\/v2\/media?parent=213"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}