Where the acceleration in the direction of s. as= dV/dt, function of t. ‘as’is ‘V’isa ‘s’and cos   dz a V dV = 0, If the flow is steady, and ds ds .On substituting and dividing the equation by we can obtain Euler's equation: ρgdA,    0  dp gdz vdv Eq.(1)  The above equation is known as Euler’s equation of motion. Bernoulli’s Equation: Integrating the Eq(1) the energy head’ H of the fluid is ‘total found by adding the three types of mechanical energy possessed by the fluid at that point. H p v z    g 2g As water flows between two points, or sections of a pipeline or channel, no energy can be created or destroyed (fundamental law of physics concerning conservation of energy). If
Where ‘as’is the acceleration in the direction of s. as= dV/dt, ‘V’isa function of ‘s’and t. cos  dz a  V dV If the flow is steady, = 0, ds and ds .On substituting and dividing the equation by ρgdA, we can obtain Euler's equation: dp  gdz  vdv  0  Eq.(1)  The above equation is known as Euler’s equation of motion. Bernoulli’s Equation: Integrating the Eq(1) the ‘total energy head’ H of the fluid is found by adding the three types of mechanical energy possessed by the fluid at that point. H  p  v  z g 2g As water flows between two points, or sections of a pipeline or channel, no energy can be created or destroyed (fundamental law of physics concerning conservation of energy). If
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