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  1. The dot product of the fluid velocity and one of the Cartesian coordinate unit vectors gives the current component in that direction. For example, let’s suppose that the current is 2.88 ms -1 to the northwest and upwelling at 0.01 cm s -1. gives the northward component of the fluid velocity.

  2. Flow Rate and Conservation of Mass. 1. cross-sectional area oriented normal to velocity vector (simple case where V ⊥ A) U = constant: Q = volume flux = UA [m/s × m2 = m3/s] U ≠ constant: Q = ∫ UdA. A. Similarly the mass flux = m = ∫ ρ UdA. A.

  3. Mathematical Tools. In this chapter we introduce a few mathematical tools that we will use in formulating some of the analysis of fluid flow problems for both inviscid and viscous flows. We introduce the use of tensor notation which is widely used in expressing fluid mechanics governing equations.

  4. The flow filed is the most important variable in the fluid mechanics, i.e., knowledge of the velocity vector filed is equivalent to solving a fluid flow problem. The acceleration vector field can be calculated: ,,, . where the compact dot products is: .

  5. Notice that [latex]\boldsymbol{V}\cdot \hat{n}[/latex] is the dot product between the velocity and outward normal that results in a scalar whose value represents the projection of the velocity vector in the [latex]\hat{n}[/latex] direction.

  6. May 11, 2022 · Recall that the dot product \(\mathbf {v}\cdot \mathbf {n}\) provides the component of the flow velocity vector \(\mathbf {v}\) aligned with the outward normal vector \(\mathbf {n}\). The mass flux allows us to keep track of the change in mass within the control volume V with time.

  7. Unlike angular momentum or angular velocity, circulation can be computed without reference to an axis of rotation; it can thus be used to characterize fluid rotation in situations where “angular velocity” is not defined easily. Solid Body Rotation.