When you pour yourself a glass of juice, the liquid flows freely and quickly. But when you pour syrup on your pancakes, that liquid flows slowly and sticks to the pitcher. The difference is fluid friction, both within the fluid itself and between the fluid and its surroundings. We call this property of fluids viscosity. Juice has low viscosity, whereas syrup has high viscosity. In the previous sections we have considered ideal fluids with little or no viscosity. In this section, we will investigate what factors, including viscosity, affect the rate of fluid flow.

The precise definition of viscosity is based on laminar, or nonturbulent, flow. Before we can define viscosity, then, we need to define laminar flow and turbulent flow. Figure 1 shows both types of flow. Laminar flow is characterized by the smooth flow of the fluid in layers that do not mix. Turbulent flow, or turbulence, is characterized by eddies and swirls that mix layers of fluid together.

Figure 1: Smoke rises smoothly for a while and then begins to form swirls and eddies. The smooth flow is called laminar flow, whereas the swirls and eddies typify turbulent flow. If you watch the smoke (being careful not to breathe on it), you will notice that it rises more rapidly when flowing smoothly than after it becomes turbulent, implying that turbulence poses more resistance to flow. (credit: Creativity103)

Figure 2 shows schematically how laminar and turbulent flow differ. Layers flow without mixing when flow is laminar. When there is turbulence, the layers mix, and there are significant velocities in directions other than the overall direction of flow. The lines that are shown in many illustrations are the paths followed by small volumes of fluids. These are called streamlines. Streamlines are smooth and continuous when flow is laminar, but break up and mix when flow is turbulent. Turbulence has two main causes. First, any obstruction or sharp corner, such as in a faucet, creates turbulence by imparting velocities perpendicular to the flow. Second, high speeds cause turbulence. The drag both between adjacent layers of fluid and between the fluid and its surroundings forms swirls and eddies, if the speed is great enough. We shall concentrate on laminar flow for the remainder of this section, leaving certain aspects of turbulence for later sections.

Figure 2: (a) Laminar flow occurs in layers without mixing. Notice that viscosity causes drag between layers as well as with the fixed surface. (b) An obstruction in the vessel produces turbulence. Turbulent flow mixes the fluid. There is more interaction, greater heating, and more resistance than in laminar flow.

Figure 3 shows how viscosity is measured for a fluid. Two parallel plates have the specific fluid between them. The bottom plate is held fixed, while the top plate is moved to the right, dragging fluid with it. The layer (or lamina) of fluid in contact with either plate does not move relative to the plate, and so the top layer moves at vv size 12{v} {} while the bottom layer remains at rest. Each successive layer from the top down exerts a force on the one below it, trying to drag it along, producing a continuous variation in speed from vv size 12{v} {} to 0 as shown. Care is taken to insure that the flow is laminar; that is, the layers do not mix. The motion in Figure 3 is like a continuous shearing motion. Fluids have zero shear strength, but the rate at which they are sheared is related to the same geometrical factors AA size 12{A} {} and LL size 12{L} {} as is shear deformation for solids.

Figure 3: The graphic shows laminar flow of fluid between two plates of area AA size 12{A} {}. The bottom plate is fixed. When the top plate is pushed to the right, it drags the fluid along with it.

A force FF size 12{F} {} is required to keep the top plate in Figure 3 moving at a constant velocity vv size 12{v} {}, and experiments have shown that this force depends on four factors. First, FF size 12{F} {} is directly proportional to vv size 12{v} {} (until the speed is so high that turbulence occurs—then a much larger force is needed, and it has a more complicated dependence on vv size 12{v} {}). Second, FF size 12{F} {} is proportional to the area AA size 12{A} {} of the plate. This relationship seems reasonable, since AA size 12{A} {} is directly proportional to the amount of fluid being moved. Third, FF size 12{F} {} is inversely proportional to the distance between the plates LL size 12{L} {}. This relationship is also reasonable; LL size 12{L} {} is like a lever arm, and the greater the lever arm, the less force that is needed. Fourth, FF size 12{F} {} is directly proportional to the coefficient of viscosity, ηη size 12{η} {}. The greater the viscosity, the greater the force required. These dependencies are combined into the equation

which gives us a working definition of fluid viscosity ηη size 12{η} {}. Solving for ηη size 12{η} {} gives

which defines viscosity in terms of how it is measured. The SI unit of viscosity is N⋅m/[(m/s)m2]=(N/m2)s or Pa⋅sN⋅m/[(m/s)m2]=(N/m2)s or Pa⋅s size 12{N cdot "m/" \[ \( "m/s" \) m rSup { size 8{2} } \] = \( "N/m" rSup { size 8{2} } \) "sorPa" cdot s} {}. Table 1 lists the coefficients of viscosity for various fluids.

Viscosity varies from one fluid to another by several orders of magnitude. As you might expect, the viscosities of gases are much less than those of liquids, and these viscosities are often temperature dependent. The viscosity of blood can be reduced by aspirin consumption, allowing it to flow more easily around the body. (When used over the long term in low doses, aspirin can help prevent heart attacks, and reduce the risk of blood clotting.)

What causes flow? The answer, not surprisingly, is pressure difference. In fact, there is a very simple relationship between horizontal flow and pressure. Flow rate QQ size 12{Q} {} is in the direction from high to low pressure. The greater the pressure differential between two points, the greater the flow rate. This relationship can be stated as

where P1P1 size 12{P rSub { size 8{1} } } {} and P2P2 size 12{P rSub { size 8{2} } } {} are the pressures at two points, such as at either end of a tube, and RR size 12{R} {} is the resistance to flow. The resistance RR size 12{R} {} includes everything, except pressure, that affects flow rate. For example, RR size 12{R} {} is greater for a long tube than for a short one. The greater the viscosity of a fluid, the greater the value of RR size 12{R} {}. Turbulence greatly increases RR size 12{R} {}, whereas increasing the diameter of a tube decreases RR size 12{R} {}.

If viscosity is zero, the fluid is frictionless and the resistance to flow is also zero. Comparing frictionless flow in a tube to viscous flow, as in Figure 4, we see that for a viscous fluid, speed is greatest at midstream because of drag at the boundaries. We can see the effect of viscosity in a Bunsen burner flame, even though the viscosity of natural gas is small.

The resistance RR size 12{R} {} to laminar flow of an incompressible fluid having viscosity ηη size 12{η} {} through a horizontal tube of uniform radius rr size 12{r} {} and length ll size 12{l} {}, such as the one in Figure 5, is given by

This equation is called Poiseuille’s law for resistance after the French scientist J. L. Poiseuille (1799–1869), who derived it in an attempt to understand the flow of blood, an often turbulent fluid.

Figure 4: (a) If fluid flow in a tube has negligible resistance, the speed is the same all across the tube. (b) When a viscous fluid flows through a tube, its speed at the walls is zero, increasing steadily to its maximum at the center of the tube. (c) The shape of the Bunsen burner flame is due to the velocity profile across the tube. (credit: Jason Woodhead)

Let us examine Poiseuille’s expression for RR size 12{R} {} to see if it makes good intuitive sense. We see that resistance is directly proportional to both fluid viscosity ηη size 12{η} {} and the length ll size 12{l} {} of a tube. After all, both of these directly affect the amount of friction encountered—the greater either is, the greater the resistance and the smaller the flow. The radius rr size 12{r} {} of a tube affects the resistance, which again makes sense, because the greater the radius, the greater the flow (all other factors remaining the same). But it is surprising that rr size 12{r} {} is raised to the fourth power in Poiseuille’s law. This exponent means that any change in the radius of a tube has a very large effect on resistance. For example, doubling the radius of a tube decreases resistance by a factor of 24=1624=16 size 12{2 rSup { size 8{4} } ="16"} {}.

Taken together, Q=P2−P1RQ=P2−P1R size 12{Q= { {P rSub { size 8{2} } - P rSub { size 8{1} } } over {R} } } {} and R=8ηlπr4R=8ηlπr4 size 12{R= { {8ηl} over {π`r rSup { size 8{4} } } } } {} give the following expression for flow rate:

This equation describes laminar flow through a tube. It is sometimes called Poiseuille’s law for laminar flow, or simply Poiseuille’s law.

The circulatory system provides many examples of Poiseuille’s law in action—with blood flow regulated by changes in vessel size and blood pressure. Blood vessels are not rigid but elastic. Adjustments to blood flow are primarily made by varying the size of the vessels, since the resistance is so sensitive to the radius. During vigorous exercise, blood vessels are selectively dilated to important muscles and organs and blood pressure increases. This creates both greater overall blood flow and increased flow to specific areas. Conversely, decreases in vessel radii, perhaps from plaques in the arteries, can greatly reduce blood flow. If a vessel’s radius is reduced by only 5% (to 0.95 of its original value), the flow rate is reduced to about (0.95)4=0.81(0.95)4=0.81 size 12{ \( 0 "." "95" \) rSup { size 8{4} } =0 "." "81"} {} of its original value. A 19% decrease in flow is caused by a 5% decrease in radius. The body may compensate by increasing blood pressure by 19%, but this presents hazards to the heart and any vessel that has weakened walls. Another example comes from automobile engine oil. If you have a car with an oil pressure gauge, you may notice that oil pressure is high when the engine is cold. Motor oil has greater viscosity when cold than when warm, and so pressure must be greater to pump the same amount of cold oil.

Figure 5: Poiseuille’s law applies to laminar flow of an incompressible fluid of viscosity ηη size 12{η} {} through a tube of length ll size 12{l} {} and radius rr size 12{r} {}. The direction of flow is from greater to lower pressure. Flow rate QQ size 12{Q} {} is directly proportional to the pressure difference P2−P1P2−P1 size 12{P rSub { size 8{2} } - P rSub { size 8{1} } } {}, and inversely proportional to the length ll size 12{l} {} of the tube and viscosity ηη size 12{η} {} of the fluid. Flow rate increases with r4r4 size 12{r rSup { size 8{4} } } {}, the fourth power of the radius.

You may have noticed that water pressure in your home might be lower than normal on hot summer days when there is more use. This pressure drop occurs in the water main before it reaches your home. Let us consider flow through the water main as illustrated in Figure 6. We can understand why the pressure P1P1 size 12{P rSub { size 8{1} } } {} to the home drops during times of heavy use by rearranging

to

where, in this case, P2P2 size 12{P rSub { size 8{2} } } {} is the pressure at the water works and RR size 12{R} {} is the resistance of the water main. During times of heavy use, the flow rate QQ size 12{Q} {} is large. This means that P2−P1P2−P1 size 12{P rSub { size 8{2} } - P rSub { size 8{1} } } {} must also be large. Thus P1P1 size 12{P rSub { size 8{1} } } {} must decrease. It is correct to think of flow and resistance as causing the pressure to drop from P2P2 size 12{P rSub { size 8{2} } } {} to P1P1 size 12{P rSub { size 8{1} } } {}. P2−P1=RQP2−P1=RQ size 12{P rSub { size 8{2} } - P rSub { size 8{1} } =R`Q} {} is valid for both laminar and turbulent flows.

Figure 6: During times of heavy use, there is a significant pressure drop in a water main, and P 1 P 1 supplied to users is significantly less than P 2 P 2 created at the water works. If the flow is very small, then the pressure drop is negligible, and P2≈P1P2≈P1 size 12{P rSub { size 8{2} } approx P rSub { size 8{1} } } {}.

We can use P2−P1=RQP2−P1=RQ size 12{P rSub { size 8{2} } - P rSub { size 8{1} } =R`Q} {} to analyze pressure drops occurring in more complex systems in which the tube radius is not the same everywhere. Resistance will be much greater in narrow places, such as an obstructed coronary artery. For a given flow rate QQ size 12{Q} {}, the pressure drop will be greatest where the tube is most narrow. This is how water faucets control flow. Additionally, RR size 12{Q} {} is greatly increased by turbulence, and a constriction that creates turbulence greatly reduces the pressure downstream. Plaque in an artery reduces pressure and hence flow, both by its resistance and by the turbulence it creates.

Figure 7 is a schematic of the human circulatory system, showing average blood pressures in its major parts for an adult at rest. Pressure created by the heart’s two pumps, the right and left ventricles, is reduced by the resistance of the blood vessels as the blood flows through them. The left ventricle increases arterial blood pressure that drives the flow of blood through all parts of the body except the lungs. The right ventricle receives the lower pressure blood from two major veins and pumps it through the lungs for gas exchange with atmospheric gases – the disposal of carbon dioxide from the blood and the replenishment of oxygen. Only one major organ is shown schematically, with typical branching of arteries to ever smaller vessels, the smallest of which are the capillaries, and rejoining of small veins into larger ones. Similar branching takes place in a variety of organs in the body, and the circulatory system has considerable flexibility in flow regulation to these organs by the dilation and constriction of the arteries leading to them and the capillaries within them. The sensitivity of flow to tube radius makes this flexibility possible over a large range of flow rates.

Figure 7: Schematic of the circulatory system. Pressure difference is created by the two pumps in the heart and is reduced by resistance in the vessels. Branching of vessels into capillaries allows blood to reach individual cells and exchange substances, such as oxygen and waste products, with them. The system has an impressive ability to regulate flow to individual organs, accomplished largely by varying vessel diameters.

Each branching of larger vessels into smaller vessels increases the total cross-sectional area of the tubes through which the blood flows. For example, an artery with a cross section of 1cm21cm2 size 12{1`"cm" rSup { size 8{2} } } {} may branch into 20 smaller arteries, each with cross sections of 0.5cm20.5cm2 size 12{0 "." 5`"cm" rSup { size 8{2} } } {}, with a total of 10cm210cm2 size 12{"10"`"cm" rSup { size 8{2} } } {}. In that manner, the resistance of the branchings is reduced so that pressure is not entirely lost. Moreover, because Q=A v ¯ Q=A v ¯ size 12{Q=A { bar {v}}} {} and A A increases through branching, the average velocity of the blood in the smaller vessels is reduced. The blood velocity in the aorta (diameter=1cmdiameter=1cm size 12{"diameter"=1`"cm"} {}) is about 25 cm/s, while in the capillaries ( 20 μm 20 μm in diameter) the velocity is about 1 mm/s. This reduced velocity allows the blood to exchange substances with the cells in the capillaries and alveoli in particular.