College Physics for AP® Courses

# 12.1Flow Rate and Its Relation to Velocity

College Physics for AP® Courses12.1 Flow Rate and Its Relation to Velocity

## Learning Objectives

By the end of this section, you will be able to:

• Calculate flow rate.
• Define units of volume.
• Describe incompressible fluids.
• Explain the consequences of the equation of continuity.

The information presented in this section supports the following AP® learning objectives and science practices:

• 5.F.1.1 The student is able to make calculations of quantities related to flow of a fluid, using mass conservation principles (the continuity equation). (S.P. 6.4, 7.2)

Flow rate $QQ size 12{Q} {}$ is defined to be the volume of fluid passing by some location through an area during a period of time, as seen in Figure 12.2. In symbols, this can be written as

$Q=Vt,Q=Vt, size 12{Q= { {V} over {t} } } {}$
12.1

where $VV size 12{V} {}$ is the volume and $tt size 12{t} {}$ is the elapsed time.

The SI unit for flow rate is $m3/sm3/s size 12{m rSup { size 8{3} } "/s"} {}$, but a number of other units for $QQ size 12{Q} {}$ are in common use. For example, the heart of a resting adult pumps blood at a rate of 5.00 liters per minute (L/min). Note that a liter (L) is 1/1000 of a cubic meter or 1000 cubic centimeters ($10−3m310−3m3 size 12{"10" rSup { size 8{ - 3} } m rSup { size 8{3} } } {}$ or $103cm3103cm3 size 12{"10" rSup { size 8{3} } "cm" rSup { size 8{3} } } {}$). In this text we shall use whatever metric units are most convenient for a given situation.

Figure 12.2 Flow rate is the volume of fluid per unit time flowing past a point through the area $AA size 12{A} {}$. Here the shaded cylinder of fluid flows past point $PP size 12{P} {}$ in a uniform pipe in time $tt size 12{t} {}$. The volume of the cylinder is $AdAd size 12{ ital "Ad"} {}$ and the average velocity is $v ¯ =d/t v ¯ =d/t size 12{ {overline {v}} =d/t} {}$ so that the flow rate is $Q=Ad/t=A v ¯ Q=Ad/t=A v ¯ size 12{Q= ital "Ad"/t=A {overline {v}} } {}$.

## Example 12.1

### Calculating Volume from Flow Rate: The Heart Pumps a Lot of Blood in a Lifetime

How many cubic meters of blood does the heart pump in a 75-year lifetime, assuming the average flow rate is 5.00 L/min?

### Strategy

Time and flow rate $QQ size 12{Q} {}$ are given, and so the volume $VV size 12{V} {}$ can be calculated from the definition of flow rate.

### Solution

Solving $Q=V/tQ=V/t size 12{Q=V/t} {}$ for volume gives

$V=Qt.V=Qt. size 12{V= ital "Qt"} {}$
12.2

Substituting known values yields

V = 5.00L1 min(75y)1m3103L5.26×105miny = 2.0×105 m3. V = 5.00L1 min(75y)1m3103L5.26×105miny = 2.0×105 m3. alignl { stack { size 12{V= left ( { {5 "." "00"" L"} over {"1 min"} } right ) $$"75"" y"$$ left ( { {1" m" rSup { size 8{3} } } over {"10" rSup { size 8{3} } " L"} } right ) left (5 "." "26" times "10" rSup { size 8{5} } { {"min"} over {y} } right )} {} # " "=2 "." 0 times "10" rSup { size 8{5} } " m" rSup { size 8{3} } {} } } {}
12.3

### Discussion

This amount is about 200,000 tons of blood. For comparison, this value is equivalent to about 200 times the volume of water contained in a 6-lane 50-m lap pool.

Flow rate and velocity are related, but quite different, physical quantities. To make the distinction clear, think about the flow rate of a river. The greater the velocity of the water, the greater the flow rate of the river. But flow rate also depends on the size of the river. A rapid mountain stream carries far less water than the Amazon River in Brazil, for example. The precise relationship between flow rate $QQ size 12{Q} {}$ and velocity $v ¯ v ¯ size 12{ {overline {v}} } {}$ is

$Q = A v ¯ , Q = A v ¯ , size 12{Q=A {overline {v}} } {}$
12.4

where $AA size 12{A} {}$ is the cross-sectional area and $v ¯ v ¯ size 12{ {overline {v}} } {}$ is the average velocity. This equation seems logical enough. The relationship tells us that flow rate is directly proportional to both the magnitude of the average velocity (hereafter referred to as the speed) and the size of a river, pipe, or other conduit. The larger the conduit, the greater its cross-sectional area. Figure 12.2 illustrates how this relationship is obtained. The shaded cylinder has a volume

$V=Ad,V=Ad, size 12{V= ital "Ad"} {}$
12.5

which flows past the point $PP size 12{P} {}$ in a time $tt size 12{t} {}$. Dividing both sides of this relationship by $tt size 12{t} {}$ gives

$Vt=Adt.Vt=Adt. size 12{ { {V} over {t} } = { { ital "Ad"} over {t} } } {}$
12.6

We note that $Q=V/tQ=V/t size 12{Q=V/t} {}$ and the average speed is $v ¯ =d/t v ¯ =d/t size 12{ {overline {v}} =d/t} {}$. Thus the equation becomes $Q=A v ¯ Q=A v ¯ size 12{Q=A {overline {v}} } {}$.

Figure 12.3 shows an incompressible fluid flowing along a pipe of decreasing radius. Because the fluid is incompressible, the same amount of fluid must flow past any point in the tube in a given time to ensure continuity of flow. In this case, because the cross-sectional area of the pipe decreases, the velocity must necessarily increase. This logic can be extended to say that the flow rate must be the same at all points along the pipe. In particular, for points 1 and 2,

$Q 1 = Q 2 A 1 v ¯ 1 = A 2 v ¯ 2 } . Q 1 = Q 2 A 1 v ¯ 1 = A 2 v ¯ 2 } . size 12{ left none matrix { Q rSub { size 8{1} } =Q rSub { size 8{2} } {} ## A rSub { size 8{1} } {overline {v rSub { size 8{1} } }} =A rSub { size 8{2} } {overline {v rSub { size 8{2} } }} } right rbrace "." } {}$
12.7

This is called the equation of continuity and is valid for any incompressible fluid. The consequences of the equation of continuity can be observed when water flows from a hose into a narrow spray nozzle: it emerges with a large speed—that is the purpose of the nozzle. Conversely, when a river empties into one end of a reservoir, the water slows considerably, perhaps picking up speed again when it leaves the other end of the reservoir. In other words, speed increases when cross-sectional area decreases, and speed decreases when cross-sectional area increases.

Figure 12.3 When a tube narrows, the same volume occupies a greater length. For the same volume to pass points 1 and 2 in a given time, the speed must be greater at point 2. The process is exactly reversible. If the fluid flows in the opposite direction, its speed will decrease when the tube widens. (Note that the relative volumes of the two cylinders and the corresponding velocity vector arrows are not drawn to scale.)

Since liquids are essentially incompressible, the equation of continuity is valid for all liquids. However, gases are compressible, and so the equation must be applied with caution to gases if they are subjected to compression or expansion.

## Making Connections: Incompressible Fluid

The continuity equation tells us that the flow rate must be the same throughout an incompressible fluid. The flow rate, Q, has units of volume per unit time (m3/s). Another way to think about it would be as a conservation principle, that the volume of fluid flowing past any point in a given amount of time must be conserved throughout the fluid.

For incompressible fluids, we can also say that the mass flowing past any point in a given amount of time must also be conserved. That is because the mass of a given volume of fluid is just the density of the fluid multiplied by the volume:

$m=ρVm=ρV$
12.8

When we say a fluid is incompressible, we mean that the density of the fluid does not change. Every cubic meter of fluid has the same number of particles. There is no room to add more particles, nor is the fluid allowed to expand so that the particles will spread out. Since the density is constant, we can express the conservation principle as follows for any two regions of fluid flow, starting with the continuity equation:

12.9
12.10
12.11

More generally, we say that the mass flow rate $(ΔmΔt)(ΔmΔt)$ is conserved.

## Example 12.2

### Calculating Fluid Speed: Speed Increases When a Tube Narrows

A nozzle with a radius of 0.250 cm is attached to a garden hose with a radius of 0.900 cm. The flow rate through hose and nozzle is 0.500 L/s. Calculate the speed of the water (a) in the hose and (b) in the nozzle.

### Strategy

We can use the relationship between flow rate and speed to find both velocities. We will use the subscript 1 for the hose and 2 for the nozzle.

### Solution for (a)

First, we solve $Q=A v ¯ Q=A v ¯ size 12{Q=A {overline {v}} } {}$ for $v1v1 size 12{v rSub { size 8{1} } } {}$ and note that the cross-sectional area is $A=πr2A=πr2 size 12{A=πr rSup { size 8{2} } } {}$, yielding

$v ¯ 1=QA1=Q πr 1 2 . v ¯ 1=QA1=Q πr 1 2 . size 12{ {overline {v rSub { size 8{1} } }} = { {Q} over {A rSub { size 8{1} } } } = { {Q} over {πr rSub { size 8{1} rSup { size 8{2} } } } } } {}$
12.12

Substituting known values and making appropriate unit conversions yields

$v ¯ 1=(0.500L/s)(10−3m3/L)π(9.00×10−3m)2=1.96m/s. v ¯ 1=(0.500L/s)(10−3m3/L)π(9.00×10−3m)2=1.96m/s. size 12{ {overline {v rSub { size 8{1} } }} = { { $$0 "." "500"" L/s"$$ $$"10" rSup { size 8{ - 3} } " m" rSup { size 8{3} } /L$$ } over {π $$9 "." "00" times "10" rSup { size 8{ - 3} } " m"$$ rSup { size 8{2} } } } =1 "." "96"" m/s"} {}$
12.13

### Solution for (b)

We could repeat this calculation to find the speed in the nozzle $v ¯ 2 v ¯ 2 size 12{ {overline {v rSub { size 8{2} } }} } {}$, but we will use the equation of continuity to give a somewhat different insight. Using the equation which states

$A1 v ¯ 1=A2 v ¯ 2,A1 v ¯ 1=A2 v ¯ 2, size 12{A rSub { size 8{1} } {overline {v rSub { size 8{1} } }} =A rSub { size 8{2} } {overline {v rSub { size 8{2} } }} } {}$
12.14

solving for $v ¯ 2 v ¯ 2 size 12{ {overline {v rSub { size 8{2} } }} } {}$ and substituting $πr2πr2 size 12{πr rSup { size 8{2} } } {}$ for the cross-sectional area yields

$v ¯ 2=A1A2 v ¯ 1= πr 1 2 πr 2 2 v ¯ 1=r12r22 v ¯ 1. v ¯ 2=A1A2 v ¯ 1= πr 1 2 πr 2 2 v ¯ 1=r12r22 v ¯ 1. size 12{ {overline {v rSub { size 8{2} } }} = { {A rSub { size 8{1} } } over {A rSub { size 8{2} } } } {overline {v rSub { size 8{1} } }} = { {πr rSub { size 8{1} rSup { size 8{2} } } } over {πr rSub { size 8{2} rSup { size 8{2} } } } } {overline {v rSub { size 8{1} } }} = { {r rSub { size 8{1} rSup { size 8{2} } } } over {r rSub { size 8{2} rSup { size 8{2} } } } } {overline {v rSub { size 8{1} } }} } {}$
12.15

Substituting known values,

$v ¯ 2=(0.900cm)2(0.250cm)21.96m/s=25.5 m/s. v ¯ 2=(0.900cm)2(0.250cm)21.96m/s=25.5 m/s. size 12{ {overline {v rSub { size 8{2} } }} = { { $$0 "." "900"" cm"$$ rSup { size 8{2} } } over { $$0 "." "250"" cm"$$ rSup { size 8{2} } } } 1 "." "96"" m/s"="25" "." "5 m/s"} {}$
12.16

### Discussion

A speed of 1.96 m/s is about right for water emerging from a nozzleless hose. The nozzle produces a considerably faster stream merely by constricting the flow to a narrower tube.

## Making Connections: Different-Sized Pipes

For incompressible fluids, the density of the fluid remains constant throughout, no matter the flow rate or the size of the opening through which the fluid flows. We say that, to ensure continuity of flow, the amount of fluid that flows past any point is constant. That amount can be measured by either volume or mass.

Flow rate has units of volume/time (m3/s or L/s). Mass flow rate $( Δm Δt ) ( Δm Δt )$ has units of mass/time (kg/s) and can be calculated from the flow rate by using the density:

12.17

The average mass flow rate can be found from the flow rate:

12.18

Suppose that crude oil with a density of 880 kg/m3 is flowing through a pipe with a diameter of 55 cm and a speed of 1.8 m/s. Calculate the new speed of the crude oil when the pipe narrows to a new diameter of 31 cm, and calculate the mass flow rate in both sections of the pipe, assuming the density of the oil is constant throughout the pipe.

Solution: To calculate the new speed, we simply use the continuity equation.

Since the cross section of a pipe is a circle, the area of each cross section can be found as follows:

For the larger pipe:

12.19

For the smaller pipe:

12.20

So the larger part of the pipe (A1) has a cross-sectional area of 0.238 m2, and the smaller part of the pipe (A2) has a cross-sectional area of 0.0755 m2. The continuity equation tells us that the oil will flow faster through the portion of the pipe with the smaller cross-sectional area. Using the continuity equation, we get

12.21
12.22

So we find that the oil is flowing at a speed of 1.8 m/s through the larger section of the pipe (A1), and it is flowing much faster (5.7 m/s) through the smaller section (A2).

The mass flow rate in both sections should be the same.

For the larger portion of the pipe:

12.23

For the smaller portion of the pipe:

12.24

And so mass is conserved throughout the pipe. Every second, 380 kg of oil flows out of the larger portion of the pipe, and 380 kg of oil flows into the smaller portion of the pipe.

The solution to the last part of the example shows that speed is inversely proportional to the square of the radius of the tube, making for large effects when radius varies. We can blow out a candle at quite a distance, for example, by pursing our lips, whereas blowing on a candle with our mouth wide open is quite ineffective.

In many situations, including in the cardiovascular system, branching of the flow occurs. The blood is pumped from the heart into arteries that subdivide into smaller arteries (arterioles) which branch into very fine vessels called capillaries. In this situation, continuity of flow is maintained but it is the sum of the flow rates in each of the branches in any portion along the tube that is maintained. The equation of continuity in a more general form becomes

$n1A1 v ¯ 1=n2A2 v ¯ 2,n1A1 v ¯ 1=n2A2 v ¯ 2, size 12{n rSub { size 8{1} } A rSub { size 8{1} } {overline {v rSub { size 8{1} } }} =n rSub { size 8{2} } A rSub { size 8{2} } {overline {v rSub { size 8{2} } }} } {}$
12.25

where $n1n1 size 12{n rSub { size 8{1} } } {}$ and $n2n2 size 12{n rSub { size 8{2} } } {}$ are the number of branches in each of the sections along the tube.

## Example 12.3

### Calculating Flow Speed and Vessel Diameter: Branching in the Cardiovascular System

The aorta is the principal blood vessel through which blood leaves the heart in order to circulate around the body. (a) Calculate the average speed of the blood in the aorta if the flow rate is 5.0 L/min. The aorta has a radius of 10 mm. (b) Blood also flows through smaller blood vessels known as capillaries. When the rate of blood flow in the aorta is 5.0 L/min, the speed of blood in the capillaries is about 0.33 mm/s. Given that the average diameter of a capillary is $8.0μm8.0μm$, calculate the number of capillaries in the blood circulatory system.

### Strategy

We can use $Q=A v ¯ Q=A v ¯ size 12{Q=A {overline {v}} } {}$ to calculate the speed of flow in the aorta and then use the general form of the equation of continuity to calculate the number of capillaries as all of the other variables are known.

### Solution for (a)

The flow rate is given by $Q=A v ¯ Q=A v ¯ size 12{Q=A {overline {v}} } {}$ or $v ¯ =Qπr2 v ¯ =Qπr2 size 12{ {overline {v}} = { {Q} over {πr rSup { size 8{2} } } } } {}$ for a cylindrical vessel.

Substituting the known values (converted to units of meters and seconds) gives

$v ¯ = 5.0 L/min 10 − 3 m 3 /L 1 min/ 60 s π 0 . 010 m 2 = 0 . 27 m/s . v ¯ = 5.0 L/min 10 − 3 m 3 /L 1 min/ 60 s π 0 . 010 m 2 = 0 . 27 m/s . size 12{ { bar {v}}= { { left (5 "." 0"L/min" right ) left ("10" rSup { size 8{ - 3} } m rSup { size 8{3} } "/L" right ) left (1"min/""60"s right )} over {π left (0 "." "010 m" right ) rSup { size 8{2} } } } =0 "." "27"`"m/s"} {}$
12.26

### Solution for (b)

Using $n1A1 v ¯ 1=n2A2 v ¯ 1n1A1 v ¯ 1=n2A2 v ¯ 1 size 12{n rSub { size 8{1} } A rSub { size 8{1} } {overline {v rSub { size 8{1} } }} =n rSub { size 8{2} } A rSub { size 8{2} } {overline {v rSub { size 8{2} } }} } {}$, assigning the subscript 1 to the aorta and 2 to the capillaries, and solving for $n2n2 size 12{n rSub { size 8{2} } } {}$ (the number of capillaries) gives $n2= n 1 A 1 v ¯ 1 A 2 v ¯ 2 n2= n 1 A 1 v ¯ 1 A 2 v ¯ 2$. Converting all quantities to units of meters and seconds and substituting into the equation above gives

$n 2 = 1 π 10 × 10 − 3 m 2 0.27 m/s π 4.0 × 10 − 6 m 2 0.33 × 10 − 3 m/s = 5.0 × 10 9 capillaries . n 2 = 1 π 10 × 10 − 3 m 2 0.27 m/s π 4.0 × 10 − 6 m 2 0.33 × 10 − 3 m/s = 5.0 × 10 9 capillaries . size 12{n rSub { size 8{2} } = { { left (1 right ) left (π right ) left ("10" times "10" rSup { size 8{ - 3} } " m" right ) rSup { size 8{2} } left (0 "." "27"" m/s" right )} over { left (π right ) left (4 "." 0 times "10" rSup { size 8{ - 6} } " m" right ) rSup { size 8{2} } left (0 "." "33" times "10" rSup { size 8{ - 3} } " m/s" right )} } =5 "." 0 times "10" rSup { size 8{9} } " capillaries"} {}$
12.27

### Discussion

Note that the speed of flow in the capillaries is considerably reduced relative to the speed in the aorta due to the significant increase in the total cross-sectional area at the capillaries. This low speed is to allow sufficient time for effective exchange to occur although it is equally important for the flow not to become stationary in order to avoid the possibility of clotting. Does this large number of capillaries in the body seem reasonable? In active muscle, one finds about 200 capillaries per $mm3mm3 size 12{"mm" rSup { size 8{3} } } {}$, or about $200×106200×106 size 12{"200" times "10" rSup { size 8{6} } } {}$ per 1 kg of muscle. For 20 kg of muscle, this amounts to about $4×1094×109 size 12{4 times "10" rSup { size 8{9} } } {}$ capillaries.

## Making Connections: Syringes

A horizontally oriented hypodermic syringe has a barrel diameter of 1.2 cm and a needle diameter of 2.4 mm. A plunger pushes liquid in the barrel at a rate of 4.0 mm/s. Calculate the flow rate of liquid in both parts of the syringe (in mL/s) and the velocity of the liquid emerging from the needle.

Solution:

First, calculate the area of both parts of the syringe:

12.28
12.29

Next, we can use the continuity equation to find the velocity of the liquid in the smaller part of the barrel (v2):

12.30
12.31
12.32

Double-check the numbers to be sure that the flow rate in both parts of the syringe is the same:

12.33
12.34

Finally, by converting to mL/s:

12.35