incompressible fluid sentence in Hindi
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- Hydraulophones use an incompressible fluid, such as water, as the initial sound-producing medium, and they may also use the hydraulic fluid as a user-interface.
- Similar to Newton, but mathematically in greater detail, Bernhard Riemann assumed in 1853 that the gravitational aether is an incompressible fluid and normal matter represents sinks in this aether.
- The fundamental principles behind these designs are based on fluid dynamics : Force that is applied at one point is transmitted to another point using an incompressible fluid known as hydraulic oil.
- When anti-vibration compound is introduced to the center bores of the rolls, vibration is transferred from the solid roll structure to the incompressible fluid component of the anti-vibration compound.
- For almost any kind of realistic system, the Liouville evolution tends to " stir " the ensemble over phase space, a process analogous to the mixing of a dye in an incompressible fluid.
- Moreover, in an initially stationary incompressible fluid, there is no vorticity, and the fluid stays irrotational, hence \ nabla \ times \ textbf { u }'= 0 \,.
- During undrained shear, if the particles are surrounded by a nearly incompressible fluid such as water, then the density of the particles cannot change without drainage, but the water pressure and effective stress will change.
- For a relatively incompressible fluid such as water, TDH is simply the pressure head difference between the inlet and outlet of the pump, if measured at the same elevation and with inlet and outlet of equal diameter.
- For density in particular, the fluid in question is also relevant; seawater, for example, is considered an incompressible fluid; its density can vary with height, but much less significantly than that of air.
- In the case of an incompressible fluid, \ frac { d \ rho } { dt } = 0 ( i . e . the density following the path of a fluid element is constant ) and the equation reduces to:
- In a sphere placed in an arbitrary non-stationary flow field of viscous incompressible fluid for stick boundary conditions where the force density s calculations leads to show the generalization of Faxen's theorem to force multipole moments of arbitrary order.
- At typical velocities, the penetration process generates such enormous pressures that it may be considered hydrodynamic; to a good approximation, the jet and armor may be treated as incompressible fluids ( see, for example, ), with their material strengths ignored.
- However, as I recently learned, a medium's volume density is " inversely " proportional to the speed of sound in the medium, while the Bulk modulus, which is higher for incompressible fluids, is positively correlational to the sound speed.
- In a sphere moving in an incompressible fluid in a non-stationary flow with mixed stick-slip boundary condition where the force of density shows an expression of the Fax�n type for the total force, but the total torque and the symmetric force-dipole moment.
- A common misconception is that the head equals the fluid's energy per unit weight, while, in fact, the term with pressure does not represent any type of energy ( in the Bernoulli equation for an incompressible fluid this term represents work of pressure forces ).
- From a strictly aerodynamic point of view, the term should refer only to those side-effects arising as a result of the changes in airflow from an incompressible fluid ( similar in effect to water ) to a compressible fluid ( acting as a gas ) as the speed of sound is approached.
- However in this case it is a completely sealed system with a much denser, incompressible fluid ( water ); I doubt the same effect would even be close to the same scale in a non-sealed system such as the " hand clapping " one .-talk ) 20 : 12, 25 May 2012 ( UTC)
- The first and third terms to the Hasegawa Mima equation, which are the same as the Navier Stokes equation, are the terms introduced by adding the polarization drift . In the limit where the wavelength of a perturbation of the electric potential is much smaller than the gyroradius based on the sound speed, the Hasegawa Mima equations become the same as the two-dimensional incompressible fluid.
- Next, in an initially stationary incompressible fluid, there is no vorticity, and the fluid stays irrotational, hence \ scriptstyle \ nabla \ times \ textbf { u }'= 0 . \, In the streamfunction representation, \ scriptstyle \ nabla ^ 2 \ psi = 0 . \, Next, because of the translational invariance of the system in the " x "-direction, it is possible to make the ansatz
- This water in turn exerts additional pressure on the air bubble inside the diver; because the air inside the diver is compressible but the water is an incompressible fluid, the air's volume is decreased but the water's volume does not expand, such that the pressure external to the diver " a " ) forces the water already in the diver further inward and " b " ) drives water from outside the diver into the diver.
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