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      In common parlance, we tend to equate "fluid" with "liquid." We think of water, oil, or coffee. However, in the realm of physics and engineering, the definition is much broader. A is defined as a substance that deforms continuously under the application of shear stress, no matter how small that stress may be.

      Can the fluid be squeezed into a smaller volume?

      Before we dive into mechanics, we must answer a fundamental question: What is a fluid? In everyday language, a fluid is a liquid. In physics, however, a fluid is any substance that deforms continuously under the application of a shear stress (a force that causes layers to slide against each other).

      This is the more complex—and more useful—branch. It deals with velocity, acceleration, and the forces involved when fluids move. To describe this motion, engineers use the , which assumes that even though fluids are made of molecules, we can treat them as continuous, infinitely divisible substances.

      Viscosity is perhaps the most critical property in fluid dynamics. It is the "friction" of the fluid world. It explains why a car needs oil to lubricate its engine and why syrup pours slowly onto pancakes. Without viscosity, there would be no drag on cars, and pipes would never suffer from friction losses.

      This introduction has given you the vocabulary of fluids: viscosity, laminar vs. turbulent flow, the no-slip condition, and Bernoulli’s principle. The next time you see a river narrow or feel the wind pick up, you will no longer see just nature—you will see the elegant equations of fluid mechanics coming to life.

      Are relatively incompressible, have a fixed volume, and take the shape of their container.

      Imagine a river narrowing from a wide section to a narrow section. What happens to the water? It speeds up. The continuity equation states that the mass flowing into a pipe must equal the mass flowing out (assuming the pipe doesn't leak).

      This is the most famous equation in fluid mechanics. Bernoulli stated that in a flowing fluid, total mechanical energy remains constant. Specifically, there is a trade-off between pressure energy, kinetic energy (velocity), and potential energy (height).

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