Derivation Of Pascal's Law, Part 2

we haveed invidi now us the of and as you can are free in the anady app apption of They aree compred al app move from their position if we apply more Force we find will still not move until some liquid is out of the tube can in this only when the tuaks weon ofid namely that they are nonpr it is liquids cannot compressed that they are for work in hydraulic systems and ma can be used to in our glass to a liquid usam effect of app Aid as an UST illustra let's the with a hammer will Toom of hom us apply aimce to the coner of H water to enable us to app toid to of as app onlys of to the botom alone isid us place a we of crosssection after the apped C am we have neglected the we of the water in the container which is very compared on theid this is true for alls of the wall can bewhere onid con we were system to app theid for 100 and ayd system operating while are me uses of under we that before the is turned is at rest in awhat C up as Begins toow the and to unil the of through the can be made the will straighten we can illust known asake when was blown through it theed straighten out the tube ofer as we blowing andess was remov The Returned thebe ofe GA GS Co of the is at one and open at the theid mayow into the open of the tube when there is no liquid flowing into the tube it appears of connect scale as the is connect a systemid under ised it tends to straighten the tube out as it straight SC press of the liquid entering the tube the more it will straighten the tube out and consequently the it will move the segment gear Ames app phant this GAE into a system where known presses can be applied to it we are able Cate scale of GA tople it consists of a coning ating a and to ofid asid to counteract the pressure of the liquid a small coed that it pushes down on Theon rod and TS toose ofid as ofid oned willward com am a pointer is attach indic the amount of compression of the on the SC compress have expained known as AER the ASD usid one at each as we saw these P are free to Ace is applied to isid andnot compressed applied as the input or a and asid appid are the will as thatp a c amid isnot compressed equ amides bided by the a amid as syes of the input and output for example here we have a tu two where the amward am when we say amount or quanti of liquid what we are actually talking ofid can volumeid asides Andes will can easily seen if we think only of the amount of liquid dises and the AMF cuses the outut to these can be visualized asind colums ofid it Canen that while volumes are the the colum ofed wies upward is wider it ISE the size or of the outut increases ites will we have in F that liquids are nonpr appid of ofel and f that is ormin to all ofes were discovered in the 1th cury by a scient nam blaz Pascal and are Su in aaln as and is as pressure liid isin TOS of the ofel