## Fluid Flow & Equipment: Crash Course Engineering #13

The world isn’t perfect. No matter how hard you try to solve a problem, or

prevent one from happening, things still go wrong. That’s just how life is. And sometimes, that means your basement gets

flooded. So, what do you do? You need to get the water out, but how? Well, you’re going to need some equipment.

Some pipes. A pump. And to choose the right pump for the job,

you’ll need Bernoulli’s Principle. [Theme Music] If you’ve seen our last episode, you already

know all about fluid mechanics and the energy

transfers involved. But engineering is about more than just learning

– it’s also about using your knowledge to build

things and solve problems. Like your flooded basement. To get the water out, you’ll need a pump –

a device that’s used to move liquids, compress

gases, or force air into things like tires. In this case, obviously, you’ll want a pump

that’s designed to move liquid, and powerful enough to push all that water in

the basement somewhere else, like outside. Preferably far away. You could just pick a random pump and hope

it works, but that’s not the engineering way. To do this properly, you can calculate how powerful

your pump needs to be with the help of 18th-century

Swiss mathematician Daniel Bernoulli. There were actually eight mathematicians in the

Bernoulli family in the 17th and 18th centuries,

including Daniel’s father and two brothers. His father was especially jealous of his success. Their rivalry was so bad that when the two of

them jointly won a scientific prize, his father

banned him from the house. He also went on to plagiarize Daniel’s later

work, changing the date so it seemed like he’d

actually published it before his son. As competitive as their relationship was, it’s possible

that the challenge pushed the younger Bernoulli

to become a better innovator and mathematician. But either way, he discovered a good deal

about fluid flow in his life. He specifically wanted to understand the relationship

between the speed at which blood flows and its pressure. So to learn more, he conducted an experiment

on a pipe filled with fluid. Bernoulli noticed that when he punctured the

wall of the pipe with an open-ended straw, the height to which the fluid rose in the straw

was related to the pressure of the fluid in the pipe. Soon, physicians all over Europe were measuring

their patients’ blood pressure by sticking sharp

glass tubes directly into their arteries. Luckily for us, they’ve developed more gentle

methods since. But while the physicians of his day were being

quite the pain in the arm, Bernoulli was on to

something very important. He realized that energy was conserved in a

moving fluid. It could be converted between different forms,

like kinetic energy – the energy of motion – and potential energy, but the total energy

within the fluid would stay the same. So if one form of energy decreases, for example,

like if the fluid slows down, there has to be a corresponding increase in anotherform of energy so the total remains constant. Bernoulli’s insight was that energy could also

be converted between kinetic and potential

energy and pressure. Today, this is known as Bernoulli’s Principle, and it says

that as the speed of fluid flowing horizontally increases,

the pressure drop will decrease, and vice versa. This means that the fluid’s speed will have

an inverse relationship with its pressure, or

that as one rises, the other falls. Now, this principle only really applies to

what’s known as an isentropic flow, meaning it doesn’t involve any heat transfer,

and it’s reversible, so it can go back to its initial

state with no outside work. Or at least, close enough that you can neglect

the effects of heat transfer or irreversibility. To keep things simple, we’ll assume this

applies to our system. For Bernoulli’s Principle, the fluid also needs to flow

horizontally, or not have a drastic change in height,

because it doesn’t consider the effects of gravity. So to account for height and gravity, and apply

Bernoulli’s Principle to the design of our pump system,

we’re going to need a more general equation. Bernoulli’s Equation. There are many forms of Bernoulli’s Equation, but the one we’ll look at today relates the

pressure, speed, and height of any two points

in a steadily flowing fluid with a density ρ. Since something’s density is just its mass

divided by its volume, this equation actually

works out really neatly: On both sides of the equation, you’ll see that

we’re defining a point’s total energy per unit volume

by its pressure, plus its kinetic energy per unit volume, and then

finally adding in its potential energy per unit volume. Basically, this equation says that the total

energy of the first point is equal to the total

energy of the second point. So if, say, the two points have different speeds,

it makes sense that they’d have different pressures

or potential energy to balance out the equation. Since the total energy will be the same at

every point in the fluid, you can also write

the equation like this. It’s very similar to what we had before, but since

the total energy will always be the same, you can replace the right side of the equation

– which represents the total energy at a second

point along the pipe – with a constant. Much simpler. And it gets even simpler if the fluid only flows

horizontally – in other words, if there’s no change

in height between the points we’re comparing. That means we can cancel out the term with potential

energy, leaving us with only the pressure and the kinetic

energy per unit volume equal to a constant. By now, you’re probably wondering how we

can find out the actual value of this constant

we keep talking about. Well, we know it’s the total energy per unit volume, and

that one way to find it is to add up the pressure, kinetic

energy over volume, and potential energy over volume. But when we’re talking about a real-life

scenario with a pump involved, we have to take into account the energy

that’s being put into and lost from the system

to move the fluid. We’ve said this energy can take two forms:

work and heat. Work is what’s driving the pump. That work is what’s moving the water along,

and contributing to the total energy. But it’s not the only factor. There’s something else that we need to take

into account: friction. As water flows through the pipe, the movement

will induce stress in the fluid, which causes friction – the resistance you get when two

things slide against each other. Friction makes a system lose energy to heat,

and there’s going to be a lot of it as the water

rubs against the inside of the pipe. Now, even with the pump, the total energy

of the fluid will still be constant throughout

the pipe. Which means the changes in energy from work

and friction will need to balance out with changes

to the three forms of internal energy – so, pressure, kinetic energy, and potential energy. That’s the only way the total energy will

remain the same. Going back to Bernoulli’s Equation, we can

now modify it slightly. The first thing we’ll do is rewrite it in

terms of changes in energy: On the left side, there are the changes to

the internal forms of energy: the change in pressure, plus the change in kinetic

energy per unit volume, plus the change in potential

energy per unit volume. That’s all equal to a constant. Then, we’ll divide the whole thing by density,

which remember, is really the same as multiplying

by volume and dividing by mass. So now we’re talking about overall changes

per unit mass throughout the flow, instead

of changes per unit volume. This is what needs to balance out with the

energy added by the pump and lost to friction. So, instead of a constant, we can now say the

left side of the equation is equal to W, the work

put in to change the energy per unit mass, minus frictional losses per unit mass. Many engineers will take this equation a step

further and divide the whole thing by gravity, which gets you the value known as head – the

height to which a pump can drive the fluid. Now, the actual amount of energy lost to friction

depends on a bunch of different parameters. One of the big ones is the velocity of the

fluid. The greater its velocity, the greater the

frictional losses. It makes sense if you think about it – there’s

going to be much more intense rubbing against the

sides of the pipe if the water’s moving faster. And remember last episode when we talked about

laminar and turbulent flow? Well that matters here too, because a turbulent,

or fluctuating flow will increase the friction more

than a laminar, or smooth flow will. The length of the pipe matters, too. If there’s more pipe for the water to rub

against, it will lose more energy to friction. And then there’s roughness: the rougher

the pipe, the more friction there will be. Not to mention every valve, fitting, bend,

and intersection in the pipe, which will also

increase the friction. To figure out how powerful the pump needs

to be to get the water out of your basement – in other words, how much work it should

be capable of producing – you’ll have to

account for all of this. You’ll want to minimize friction by keeping the pipe

as simple and short as possible – this way, you won’t

need as much work to counter the energy loss. The pump also needs to be able to perform enough

work to account for the pressure and velocity of the

water, as well as any changes in elevation. Reality tends to be a little messier than the simplified

version of Bernoulli’s equation we’re using, but it should be enough to get a sense of

which pump you’ll need to finally clear out

your basement. Who knows how much mold is growing down there

by now. More generally, Bernoulli’s equation is a good

foundation for working with fluids and figuring out

how to build your designs around them. The world isn’t always perfect, but with

the right engineering skills and tools, it

doesn’t have to be. So today was all about diving further into

fluid flow and how we can use equipment to

apply our skills. We talked about Bernoulli’s Principle and

the relationship between speed and pressure

in certain flowing fluids. We then learned how to apply the principle

with Bernoulli’s Equation. Taking that equation, and substituting a constant

with work and frictional loss, gave us a great way

to use it in real-world examples. I’ll see you next time, when we’ll talk

all about heat transfer. Make sure you bring a bottle of sunscreen. Crash Course Engineering is produced in association

with PBS Digital Studios. You can head over to their channel to check

out a playlist of their latest amazing shows, like

Brain Craft, Deep Look, and PBS Space Time. Crash Course is a Complexly production and this

episode was filmed in the Doctor Cheryl C. Kinney Studio

with the help of these wonderful people. And our amazing graphics team is Thought Cafe.

At first I thought "pressure drop will decrease" means "pressure will increase". Double negatives here.

7:43 the formula shown is wrong

Amazing, your videos worth = 2 hrs of self study=1 hour class lectures.

lmfao lil pumps basement flooded