![]() ![]() This equation is also termed as “Conservation of mass of This is the equation of continuity.įrom Equation of continuity we can say that Av=constant. Volume covered by the fluid in a small interval of time ∆t,Īcross left cross-sectional is Area (I) =A 1 xv 1 x∆tĪcross right cross-sectional Area (II) = A 2 x v 2 x∆tįluid inside is incompressible (volume of fluid does notĬhange by applying pressure) that is density remains same.Īlong (I) mass=ρ 1 A 1 v 1 ∆t and along second point (II) ,īy using equation (1), we can conclude thatĪ 1 v 1 = A 2 v 2. Respectively, velocity and density of fluid at other end (II)= The velocity and density of the fluid at one end (I)=v 1, ρ 1 Let the cross-sectional area at one end (I) = A 1 and cross. Of liquid across any cross-section remains constant.Ĭonsider a fluid flowing through a tube of varying thickness. Pipe of non-uniform cross-section area, then rate of flow It means that if any liquid is flowing in streamline flow in a Where A =cross-sectional area and v=velocity ![]() According to the equation of continuity Av =Ĭonstant. ![]() PHYSICS INVESTIGATORY PROJECT 2018 – 2019 BERNOULLI’S THEOREM MADE BY: AARYA RAJESH INDEX PRESSURE EQUATION OF CONTINUITY DANIEL BERNOULLI INTRODUCTION TO BERNOULLI’S THEOREM BERNOULLI’S EQUATION EXPERIMENT APPLICATIONS EQUATION OF CONTINUITY ![]()
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