This mechanism shrinks when pulled

This little mechanism shrinks when you try to stretch it.

You try to pull it apart and all of a sudden it pulls back on you.

That's so weird, right?

Here it is under controlled conditions.

There's a cup hanging from the mechanism.

But now look what happens as you add water to it.

All of a sudden, the cup shoots up.

The amount it shoots up is tiny.

But the physics behind it is so counterintuitive,

nobody thought it was possible.

It feels like it violates physics.

That's why it's fun.

The paradox that controls this mechanism governs everything from mechanical

systems to food chains,

from traffic jams to power grids.

And to understand it, you just need to ask a simple question.

What will happen to this weight if you cut the green rope?

Where is this going to end up?

Is it going to go up?

Is it going to going to go down?

Or is it going to stay the same? Can I touch? Yeah. Yeah.

Yeah, you can try it. Nothing.

You don't think anything's going to happen?

In the same place.

Uh, weight is going to be right over there.

Like it's going to fly off or what?

No, not not too much, but probably

it's going to go to this way.

If you cut the green rope, this is going to come down.

It will go down.

It will go down. It drops. It'll fall down.

The first thing that occurs to me is as soon as you cut that,

the weight is going to drop.

I imagine the weight ends up lower than it started.

Here's a closer look at the setup.

You have a spring hanging from a hookup here.

And then via this green rope, it's connected to another spring

that's carrying this weight below them.

There are two extra ropes here as well.

So the red one and the black one are slack.

They're not under any tension whatsoever.

So they're not actually carrying any weight.

What's going to happen if you cut the green rope?

You can pause the video here and try to figure it out for yourself. Wait, what?

Here it is in slow motion.

So, even though the ropes on the side were slack and we cut the

only rope in tension,

the weight somehow went up.

Okay, so if you're unconvinced

that cutting the green rope actually

makes the weight go up, here's a huge version of the experiment.

So, the black and red ropes are still

very much slack and it's just held together by this tiny piece of green rope here.

So, let's see what happens now. Okay, you ready? Okay. Three, two, one.

That was actually insane.

That was pretty pretty good, right?

I still don't believe it looking at it.

Okay, so why does this actually happen?

Cuz the springs are contracting

back and just pulling it together.

Maybe the tension in the,

you know, this part is changed.

It releases the tension in the springs and only goes to the length of

the Look at what happens when you remove the slack side ropes from the initial setup.

You're left with this

a mass hanging from a spring hanging from another spring.

So these springs are connected in series.

Obviously when you hang a weight from one spring,

it extends just like you'd expect.

And the amount it extends by, call it X, is proportional

to the force exerted by the weight. That's Hook's law.

But if you add another spring in between in series,

now both springs extend roughly the same amount,

X, because both springs feel the same force of the weight pulling from below.

So in the case of ideal

massless springs, you would end up with exactly 2x of displacement.

Now there's another way to connect these two springs to the weight, and that is in parallel.

This way, both springs are independently

connected to the hook above and to the weight.

So, each spring is only carrying half the weight of the mass below,

which is why both springs extend only half as far or x over two.

If you look at the setup right after the green rope is cut, you'll

notice that this is actually exactly

how the springs are laid out.

So, the red rope is connecting the bottom spring directly to the hook above,

and the black rope is connecting the top spring to the weight.

So these springs are in parallel.

So by cutting the green rope, you're actually forcing the springs to go from

a series to a parallel.

And that change is what causes the contraction to happen.

When you cut the rope, each spring only extends by about half as far

as before, which is why you can add so much slack on these black

and red ropes to give the impression that the weight is going to fall down.

When you cut the rope, you go from series to parallel

and that pushes you up.

The slack ropes, that's where I get to cheat.

And that that's that's the misleading bit, you know.

Yeah, the key to getting this paradox right comes down to the length of the slack ropes.

Each one has to be longer than the length of one of the springs

in series plus the green rope.

That's what adds the slack.

But they also can't be much longer than that because too much slack will

nullify the contraction you get between series and parallel and the weight will still fall.

Now, you might think that this paradox only really works with the springs in

this demo, but the first time it was discovered was actually because of its influence on people.

In April of 1990,

New York was getting ready for its 20th annual Earth Day.

It was going to be Manhattan's

biggest celebration of environmentalism to date.

Stop the war against the Earth.

On the day, Central Park was turned into a massive festival ground with almost

a million people pouring in to see a stacked lineup of performers,

including Hallen Oats and the B-52s.

But the boldest stunt of the day was to ban traffic on some of

New York's most important streets,

including 42nd Street, one of the busiest streets in Manhattan.

It stretches from river to river connecting Time Square to Grand Central Station

and it's almost always jammed with slowmoving traffic.

The only thing that's an hour from 42nd

Street is 43rd Street.

And maybe not surprisingly,

people were really against this idea,

insisting that just a 6-hour

closure of 42nd Street would mean doomsday.

As the commissioner of New York's Department of Transportation

put it, you didn't need to be a rocket scientist or have a sophisticated

computer queuing model to see that this could have been a major problem.

But the city went ahead with it anyway,

and no cars were allowed on 42nd

Street for the day.

Now, to everyone's surprise,

the traffic in the surrounding area actually got better.

The number of cars was reduced by 20%

with bystanders claiming the whole area was a ghost town compared to the way it normally is.

But one man wasn't surprised by this result.

In fact, he predicted it over 20 years

His name was Dietrich

Braze, a German mathematician.

And back in 1968,

Braze was studying road networks.

As part of his research, he imagined a scenario where drivers from one side

of a fictional town were trying to get to the other.

But there were only two possible routes the drivers could take.

Route one starts with a wide highway that takes you halfway across town.

The road is so wide that regardless of how many cars are on it,

this part of the trip always takes 25 minutes.

The second half of this route turns into a narrow city street, and the

time to drive through this street depends on how many cars are on it.

For every 100 cars on the street, the time to pass through it takes an additional minute.

So 100 cars will take 1 minute, 200 cars will take 2 minutes, and so on.

The second route through town starts with a similar narrow city street that depends

on the number of cars.

It takes you halfway across and then turns into another 25-minute

highway stretch where the transit time doesn't depend on traffic.

So which route would you take to get across town?

Well, you can see that the routes are identical but flipped.

So, it doesn't really matter.

Since this is just a mathematical

model, both will get you there at the same time.

So, say there were 2,000

drivers trying to get across the city.

Half of the cars would end up on the first route and half on the second route.

And since there are now 1,000

cars going down each narrow city street, the travel time on these segments increases to 10 minutes.

So, the total time on both routes is 10 minutes for the narrow street

plus 25 minutes for the highway.

A total of 35 minutes regardless of route.

But now, say the city decides to connect these two routes at the halfway

point with a small piece of highway to give drivers more options.

This piece only takes a minute to travel across.

So, which roads would you use now to get across town?

Well, as an individual driver,

you should just go straight down.

It will take you 10 minutes to get through the first city street,

1 minute on the new connecting road, and another 10 minutes for the second street.

So your total journey time would now be only 21 minutes compared to the

35 minutes for everyone else on routes 1 and two. Okay, great.

So you minimize your own time and that's that, right? Well, not really.

See, drivers like you are selfish and everyone wants the shortest possible travel time,

which means everyone starts flooding

the narrow city streets.

As drivers switch to this new shortcut,

the narrow streets become more and more congested,

making the route slower and slower.

But this makes the original routes worse, too.

Because the time to get through the street segments keeps increasing for every driver.

So, everyone decides to switch to the shortcut.

And now all 2,000

cars are driving down the city streets.

Now, the time to traverse each city street jumps to 20 minutes.

So, the total journey time for everyone increases to a whopping

41 minutes compared to the 35 minutes we had before the new road was constructed.

So traffic actually got worse for everyone.

To fix it, the drivers

could simply go back to their original routes, right?

Well, who's going to be the first to switch back?

If any one driver goes back to Route 1 or two, their journey time

will be the 25 minutes on the highway plus 20 minutes on the now

congested city streets, or 45

minutes in total, which is even worse than the now congested streets.

So, no single driver would ever want to go back to the original route.

And because humans are humans, it's not like we could all just agree to

ignore this new road.

So, even though every driver was making a rational decision to try to minimize

their own travel time by just using the city streets,

collectively, this made the situation worse for everyone,

and there's no way out.

But if the city were to destroy

this new connecting road,

everyone's journey time would drop from 41 minutes back to the original 35

minutes on route 1 and two.

So removing the road

would actually make the traffic better.

It's just like cutting the green rope from before.

That's because both of these are examples

of the same paradox.

The springs are like the narrow city roads.

The more weight or cars you add,

the longer they get.

And the ropes are like the highways.

It doesn't matter how much weight is on them, they don't change.

That is unless you don't know how to tie them properly. My god.

This is the paradox Dietrich Braze discovered in 1968.

It's now known as Brazy's

paradox, and it is the reason why New York traffic got better after 42nd

Street was closed on Earth Day.

Now, sure, you'd be right to argue that the reason the traffic decreased on

Earth Day in New York was simply because people decided to walk or cycle

more that day, but it turns out mathematicians

actually modeled the whole city in 2008.

And they found 12 roads that were redundant and could be cut to actually reduce traffic.

And it's not only New York.

The paradox showed up in Boston, London, Seoul.

In fact, if you were to randomly add a new road to just about

any city, you'd have an equal chance of making the traffic better

as But there's nothing special about the flow of cars.

Say instead you want to send electricity

from one station to another.

Well, now you're looking at the flow of electrons in a power grid.

And just as before, you could try to improve the grid by increasing the

capacity of existing lines or by adding new lines.

But it turns out that this can actually destabilize

the grid or even cause a blackout.

And virtually any other network,

anytime you're sending things from one place to another, it can fall prey to Brazy's paradox.

Be it a food chain,

blockchain, or even the internet.

Adding elements to the network can make it worse.

So less can actually be more.

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I drafted up a little email,

but once I hit send,

suddenly my inbox flooded with spam emails.

Grace and Jenny offering price lists for

well, I don't really know what.

Oh, and the best email actually suggested we should turn Veritassium's

existing content into high performing YouTube videos

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and extend the brand's reach.

That's a genius idea.

But unfortunately, most of these emails are spam and I'd very much like them to stop.

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Go get it off.

What are you doing here?

Braz's paradox doesn't occur every time you modify a network.

You need a very specific set of conditions for it to occur.

But if you can make it work consistently, you get this.

So, we're here at the Amolf

Institute where they actually figured out how to make something shrink

when you pull it.

So, let's go check it out. Is it here?

Yeah, I made all these samples. That's so weird. Yeah, right.

I guess you never expect things to yank back on you so unexpectedly

cuz a rubber band, you're stretching it and you feel

it wants to pull back on you more and more, but here it just

you're never ready for freezing suddenly,

which it's a weird feeling.

There's something almost like human about it where it starts tugging back on you

when it gets bad.

What's special about this mechanism is that everything else around us works in the complete opposite way.

Try to press one of your keyboard buttons slowly so that it steadily goes down into place.

You can't do it.

No matter how slowly you go,

there is some point at which it just gives way and clicks through.

The same happens if you try to stretch a bendy straw.

You can pull on it as slowly as you like, but at some point

the individual straw joints are going to expand suddenly.

light switches, eyeglasses, grasshopper

legs, these all have a failure point beyond which they give way and quickly

snap into a different position.

And this is called well snapping.

Here it is mapped to a force displacement graph.

As you'd expect, the more force you apply, the more the material bends or displaces.

But eventually you reach a tipping point and beyond it, the force required to

bend the material further actually drops.

So if you apply a force higher than that peak, the displacement

has to rush to the next corresponding

value to match the force

which is all the way on the other side of this dip.

And as a result, you get a huge amount of displacement

for that tiny increase in force.

That's what creates the sudden snap. It's very intuitive.

I mean, you've all experienced

it, at least if you're in the Netherlands, with your umbrella.

There's a gust of wind underneath your umbrella.

It pops to the other side.

So you sort of go over a peak

in energy or in force and it suddenly snaps and typically it becomes softer.

And this is the way all things snap.

Everything used to fail in the direction of the applied force

until this mechanism came about

doing the exact opposite of snapping.

Call it counter snapping.

Imagine that gust of wind blows under your umbrella but instead of flipping out

your umbrella suddenly closes in.

Or you try to pull apart a straw and the joints suddenly contract.

The wind is pushing on my umbrella, but instead of it folding out, it

would push itself against the wind to close itself, right?

But it feels like it violates physics.

It It's just so

so counterintuitive that the displacement is in

in the other direction to the force.

That's why it's fun.

So, how does this thing work?

Well, the mechanism itself is built out of three different components,

and on their own, they all stretch normally when you try to pull them apart.

Individually, they behave like springs in the sense that they extend when you pull

on them, but then you combine them together, and then suddenly they shrink. Exactly.

If you draw the system as a set of springs,

it looks something like this.

The long and lanky components represent the two springs on the sides,

but they actually don't feel like springs at all.

You can easily pull them apart until they suddenly get very stiff.

Meanwhile, these pieces represent the top and bottom springs, and they feel a lot more springy.

So, the more you pull them, the more they pull back.

And finally, the central piece.

It looks very similar to the previous one, but pulling it apart feels very snappy.

In fact, you can even hear it snap out.

Put them all together and you get the mechanism.

If you stretch it slowly,

you'll see how tension builds up in the three middle pieces

with the sides staying mostly relaxed.

But if you keep stretching,

the centerpiece will suddenly snap out and transfer most of its tension to the side springs.

This causes the system to stiffen and shrink.

If you now let go,

the system resets, so the mechanism can flip between a set of springs in

series to one in parallel.

It's a reversible case of Brazy's paradox.

The network is basically the same as the brush paradox.

So the the way they connected, the topology of the connection is exactly the same.

The force displacement graph you get for the mechanism

is one that loops in on itself

with two distinct curves.

One for the system in series and the other for the system in parallel.

And this leads to some pretty remarkable properties.

If you slowly control the stretching force by adding water to a cup below

the mechanism, the mechanism

first slightly sags like you'd expect.

But when you reach the tipping point at the end of this curve,

the displacement has to quickly reduce to keep following the force along the graph.

And this jump back is why the mechanism shrinks.

Now you can also control displacement

instead of force and measure how much force it takes to stretch the mechanism at any point.

This time when you reach the tipping point, it's the force that has to

follow displacement along the graph.

So you get a sudden jump up in force showing that the material has stiffened.

Oh, this little force jump is enough to make it slip out of your hands.

If example, I mean it even though you said it is a small jump,

it's like this is the only

thing that does this

anywhere probably on Earth.

Uh yeah, as far as we know, the force jumping like this, it was not reported.

It is pretty insane.

So what is counter snapping actually useful for?

Well, notice that there is a force at which the series and parallel curves

of the system overlap.

Which means that at this force, the mechanism will actually be the same length in both states.

So if you exert that exact force on the structure by for example hanging

a weight from it, you can flip between the two states by giving the

mechanism a little tug.

And although that will change whether the springs are in series or parallel,

it won't change how long the system actually is.

So you can change the stiffness

without changing the length.

Now look at what happens if you give the mechanism a nudge in its original series state.

If you poke it, you it's basically a way to measure the natural frequency. Oh yeah.

When the mechanism is in series, the natural frequency is 3.7 hertz.

But if you switch to a parallel setup, the natural frequency increases to 6.4. 4 hertz.

We switch it and we look at the natural frequency.

Now we can see it's much higher.

What's unique here is that you're able to almost double the natural frequency of

the material without changing its length.

I'm going to move the robot robotic arm very slightly

just up and down. Yeah. Okay.

And I put a frequency of 3.5 hertz.

So it's close to the natural frequency of this system.

This is going to drive the structure into resonance.

But once the vibrations

get big enough, the mechanism is actually going to switch states on its own,

change its natural frequency,

and thereby reduce the vibrations.

Like it gets stronger and stronger, and then it just locks it out. Yeah. Yeah. That's cool.

The same happens in reverse.

If you vibrate the robot hand at 6.4

hertz, the mechanism is quickly going to switch back to its original state and minimize the vibrations.

It's interesting uh the way that you say it.

We're moving the point at which resonance happens.

And that's what stops excessive vibrations. Yeah. Interesting. Yeah.

Other snapping structures could also switch upon resonance.

But the problem that once they switch,

they're much more elongated, much more contracted.

So they don't, let's say, they wouldn't provide the same function.

You could use this effect to keep structures from vibrating or reaching resonance.

Could it be easier to install

a system like this where you're actually moving the resonance instead of like a

whole tune mass damper or or something like that?

Yeah, I think this solution is still very complex.

It's very complicated design, but I think the principle could be used.

I know it's still super early, but I'm really

excited to see like it pop up somewhere, you know, in a couple of years or decades.

It's more about the concept and showing what it can do.

We're going to try to see if we can maybe make contra snapping also

maybe with different type of variables.

It's going to be like a balloon that deflates when you inflate

You increase the pressure and the volume would decrease. Wait, really? That's crazy.

That would be the equivalent,

but we it's not there yet, but we'll see. That's so cool.

In principle, it should be possible. Yeah.