Cross-sectional area of the flow at point 2
{"title":"Cross-sectional area of the flow at point 1","description":"Wrong","type":"incorrect","color":"#99CCFF","code":"[{\"shape\":\"poly\",\"coords\":\"82,133\"},{\"shape\":\"rect\",\"coords\":\"2,8,40,56\"}]"} {"title":"Flow speed at point 1","description":"Incorrect","type":"incorrect","color":"#ffcc00","code":"[{\"shape\":\"rect\",\"coords\":\"118,11,119,13\"},{\"shape\":\"rect\",\"coords\":\"73,16,99,53\"}]"} {"title":"Flow speed at point 2","description":"Wrong","type":"incorrect","color":"#333300","code":"[{\"shape\":\"poly\",\"coords\":\"113,132\"},{\"shape\":\"rect\",\"coords\":\"195,33,199,34\"},{\"shape\":\"poly\",\"coords\":\"132,99\"},{\"shape\":\"rect\",\"coords\":\"249,16,283,53\"}]"} {"title":"Cross-sectional area of the flow at point 2","description":"Correct!","type":"correct","color":"#000080","code":"[{\"shape\":\"rect\",\"coords\":\"177,8,220,54\"}]"}It takes some time interval Δt for the slug of fluid to enter the region at point 1. And since the volume of fluid between the points must remain constant, the slug of fluid at point 2 must exit the region in the same time interval. If we divide Equation 11-17 by the time interval Δt it takes for the slugs of fluid to enter or exit the region, we arrive at
A1Δx1Δt=A2Δx2Δt
To see why we divided through by Δt, note that the fluid at point 1 moves a distance Δx1 during the time interval Δt and so has speed v1=Δx1/Δt. SImilarly, the fluid at point 2 (which moves a distance Δx2 during the same time interval) has speed v2=Δx2/Δt. So we can rewrite Equation 11-18 as the following relationship called the equation of continuity: