Unsolved Engineering Problem: Runaway Anchor Drops

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Runaway anchor drops remain a significant engineering challenge despite historical attempts to improve brake designs. The lack of feedback for operators can lead to dangerous situations where they mistakenly release the brake, causing the chain to accelerate uncontrollably. Suggestions for improvement include using electric drives with regenerative braking and incorporating additional safety devices like rotary fluid dampers. The discussion also highlights the need for better operator training and the potential benefits of automation, such as GPS systems to prevent accidental brake release during motion. Overall, the complexity of the problem suggests that while solutions exist, they may not be widely implemented due to tradition and conservatism in engineering practices.
  • #31
russ_watters said:
That'd be a start, but the runaway typically continues after the anchor hits the bottom. The chain is most of the weight. Maybe deployable sea anchors at regular intervals along the chain...
But does the runaway start after the anchor hits bottom?

It would be great if you could have them at multiple points on the chain, but then we introduce the tangling possibility you mentioned before.
 
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  • #32
On smaller boats the anchor rode contains a relatively small section of chain and the rest is rope. Why is this not true for the big ships? The geometry of the anchor seems scale invariant to me. I would hate to haul up 100 ft of chain on a 25 ft boat.
The big ships seem to have all chain. Strength? Fire resistance?
 
  • #33
Rive said:
Anyway. An additional point about those brakes: since the chain is supposed to be 'laid down' on the seabed, the ship is usually moving (albeit slowly) during a regular anchor drop. If the anchor got stuck after it reaches the bottom then those brakes are dealing with the mass and momentum of the whole ship, and not just with the chain itself...
No, after being set, the chain is simply being unspooled along the bottom, but stationary/with no tension beyond from its weight. There's no time when the ship has significant speed while setting/dropping the anchor, and no significant dragging occurs/is desired. The main problem would simply be dragging the anchor, not damaging the equipment. Also, the anchor can't be set if the angle is steep; it needs to be pulled horizontally. The scenario where an anchor is being dragged at significant speed on a short length of chain and then catches an obstruction would be very unusual.

And even for what it is, I don't see much chance for damage. It would require hard-setting the brake at a time when it has to be softly applied (otherwise the anchor wouldn't get to the bottom).
 
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  • #34
Wow! I asked for a good discussion and I'm getting it. More than I can deal with on a timely basis. I'll delay the power calculation to later.

erobz said:
Aquachute(s) that trigger at certain threshold accelerations using accelerometers.
As Russ Waters said, a "sea anchor." I don't think you can make one rugged enough to survive. Runaway can start both before and after the anchor hits bottom.

However, I think you're on the right track. My own thinking is leaning toward a "velocity limiter" as the best preventer of runaways. Something with a force versus velocity curve like this. It could be a backup added to existing system, not a replacement for the brakes.
1661344496534.png

A "sea anchor" is like that, but it is not very rugged. Perhaps an eddy current brake, or a hydraulic torque converter.

berkeman said:
Using friction or electromagnetic braking? Actively cooled with water? It doesn't look like it from the video...
Sorry, I must have written that poorly. Existing systems don't have electrodynamic brakes or water cooling. I meant to say that they could have those things as you suggest.
russ_watters said:
But in a properly executed, normal anchorage the ship is stationary when the anchor hits the bottom and only then starts backing down as the chain is played-out.
True, but just like any vehicle, the design must be rugged enough to handle foreseeable abuse.

russ_watters said:
That'd be a start, but the runaway typically continues after the anchor hits the bottom. The chain is most of the weight. Maybe deployable sea anchors at regular intervals along the chain...
Yes, that's right. If the runaway speed exceeds ship speed, the fall becomes vertical, and the weight suspended depends on the depth of the water.
hutchphd said:
The big ships seem to have all chain. Strength? Fire resistance?
Durability. Coral in particular cuts rope like knives. In the tropics, you'll never see a boat with rope in the ground tackle.

But also holding force in rough weather. Small displacement boats depends on the holding force of the anchor. Heavier boats depend on the holding force of that long length of chain laying on the bottom. Ideally, after deployment the horizontal pulling force on the anchor is zero. That's another mystery of anchoring. To raise the anchor, you need to pull vertically up, not horizontally.
Rive said:
With that, I imagine it would be pretty difficult to bring an ongoing runaway under control.
Exactly. So runaway prevention should be the goal, not runaway halting.

---
By the way, this video illustrates the chain runaway scenario on a micro scale. It doesn't help much in our discussion other than to illustrate how the distributed masses and momenta play roles. Note that inertia of the ascending portion of the chain is also significant.



---
Great thinking everyone. PF has many talented engineers as members.
 
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  • #35
russ_watters said:
There's no time when the ship has significant speed while setting/dropping the anchor, and no significant dragging occurs/is desired.
May not be desired, but as far as I know this is how a failed anchoring attempt looks like.
That speed might look slow but if the anchor gets stuck somewhere you'll sure have some problem on your deck.
 
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  • #37
anorlunda said:
By the way, this video illustrates the chain runaway scenario on a micro scale. It doesn't help much in our discussion other than to illustrate how the distributed masses and momenta play roles. Note that inertia of the ascending portion of the chain is also significant.
Is there a significant length of chain hanging off the backside of the capstan? I assume its piled in the bottom but hanging vertically between there and the capstan.
 
  • #38
russ_watters said:
I don't understand what you are saying here: why would the anchor brake need to stop the ship? ...and why as soon as it touches bottom?
Somebody hasn't been studying their history. The last stand of the USS Missouri in 2012 teaches us how to deploy an anchor in an emergency. :oldbiggrin:

 
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  • #39
anorlunda said:
As Russ Waters said, a "sea anchor." I don't think you can make one rugged enough to survive. Runaway can start both before and after the anchor hits bottom.
I guess the question is how large, and durable does it need to be to limit the decent velocity to a safe range. I imagine one of the sea anchors fixed to the anchor with a small buoy on top to keep it upright.

I get the following equation of motion, for what seems like would be worst case scenario...complete primary brake failure.

$$ \lambda \left( x+ l_o\right) \ddot x = \lambda g \left( x-l_o \right) - \beta { \dot x}^2 $$

Where:

##\lambda## is the chains mass per unit length
## l_o## is the length of chain suspended on the back of the capstan
## \beta## is the total drag coefficient
## \downarrow^+ x## is the length of hanging anchor

If I had the figures, I could try to solve for the projected area of the sea anchor, and force on it required to limit its velocity to some threshold.

I know you said they can start after the anchor has landed too, but how often is that the case when it is a controlled decent? If its uncontrolled, and the anchor hits bottom while the chain is carrying a lot of momentum, then the "sea anchor" doesn't help, but if the sea anchor always provides some level of controlled decent is it likely to happen?

EDIT: This model isn't quite correct either. I think there is supposed to be a linear ##\dot x## term in there as well. I remember having a conversation in PF before about the solution being somewhere between Work/Energy and Impulse/Momentum for the rising chain (on the back of the capstan) which is accelerating the links in the pile from rest...I didn't account for that

EDIT: Maybe its ok after all. That was a slightly different problem where the length of the chain rising was increasing. This problem the length of the chain rising is constant.
 
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  • #40
erobz said:
Is there a significant length of chain hanging off the backside of the capstan? I assume its piled in the bottom but hanging vertically between there and the capstan.
Chain is stored as low as possible to keep the ship's center of gravity low. So if sea level is 0, chain is stored at 0 to -15 feet. The hawse pipe where chain leaves the ship is almost at the top deck, +50-70 feet, anchoring depth of water on the continental shelf is typically 100 feet, so yes, the ascending part is a significant fraction.

Re-watch the chain fountain video carefully. At 17 seconds, the man let's go of the chain with his fingers, at about the same level as the bottom of the glass beaker. But the chain has a high velocity at the instant he let's go. The fountain starts from there. That tells me that it doesn't matter how long the distance is to the floor, but rather that velocity is the key parameter. It would be interesting to repeat that experiment with the glass beaker on a table, to see if the fountain continued if the final resting place of the chain is on the table top.

Regarding the sea anchor. First, I agree with @russ_watters, the runaway can start after the anchor hits bottom. Indeed, in some of the cases on video, the chain first stops then moves again before runaway. I interpret the stop as the time when the anchor hits bottom. Therefore, to anchor in 100 feet of water, you need another sea anchor every 100 feet of chain.

Sea anchor durability: I'm most worried about dragging the chain across the bottom. That tends to rip off anything attached to the chain.
 
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  • #41
This video is better. The capstan wheel is visible. The chain stops several times. The men on the brake are seen turning the wheel to loosen the brake for minutes. Finally, runaway begins. Here are significant events in the video.

1661377541702.png


There is so much dust in the air, that the men can not be seen trying to tighten the brake after runaway begins. However, I think they may need to turn that wheel the other direction for 3 to 4 minutes before the brake starts braking again. But the chain is lost in less than 1 minute.



I also found some data from the USS Nimitz. I'm going to try to estimate chain velocity from the videos, and then calculate braking power needed to prevent a runaway.

1661377803337.png
 
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  • #42
Anchors Away!
(Sorry couldn't resist the pun)
 
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  • #43
anorlunda said:
This video is better. The capstan wheel is visible. The chain stops several times. The men on the brake are seen turning the wheel to loosen the brake for minutes. Finally, runaway begins. Here are significant events in the video.

View attachment 313228

There is so much dust in the air, that the men can not be seen trying to tighten the brake after runaway begins. However, I think they may need to turn that wheel the other direction for 3 to 4 minutes before the brake starts braking again. But the chain is lost in less than 1 minute.



I also found some data from the USS Nimitz. I'm going to try to estimate chain velocity from the videos, and then calculate braking power needed to prevent a runaway.

View attachment 313231

I think I’ll use this data and update the model to include the buoyant force and the mass of the anchor, neglect drag for now and try to calculate the speed for some initial conditions. With any luck I’ll be in the ball park of what you find in the video.
 
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  • #44
Brake fade is another possible cause of chain runaway. The chain pull at the brake multiplied by the chain speed is a LOT of power, and thus heat generated in the brake. That heat is generated at the contacting surfaces between the brake pads and brake drum. The brake drum is almost certainly a steel alloy, possibly cast iron. I don't know what those brake pads are made from, but they are very likely a non-metallic material.

The surface temperature at the braking surface is the result of the heat generated minus the heat removed by conducting through the brake pad and drum. If the brake pad surface gets hot enough, it can vaporize. This could be the source of the (dust) (smoke) seen during the runaways. If that is what is happening, there is gas generated at the braking surface. That gas is a lubricant which causes the friction coefficient to decrease dramatically.

I once experienced brake fade. I was driving my 1961 Rambler American like a typical overconfident teenager. I came over a hill at 80 MPH, and saw a stop sign at the T intersection at the bottom. Standing on the brakes got the speed down to 25 MPH, at which point braking action ended. I was able to get around the corner by putting two wheels in the ditch to pull it around while somehow not hitting the stop sign. When brakes stop braking due to brake fade, they stop almost instantly. Brake fade is not a gradual process.

The last time I was in a private jet, the pilot landed a little fast on a short (for that airplane) runway. The brakes were smoking after he stopped. He claimed that it was a normal landing. I did not believe him, partly because that was the only time I saw those brakes smoking.
 
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  • #45
I guess the main direction will be the missing redundancy and maybe an elevator style speed limiter :smile:
 
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  • #46
May be a silly question, but would it make any difference at all if some kind of pattern is stamped on to each link of the chain that would maximize turbulence and hence drag? Analogous to engineering the surfaces of golf balls, etc ?
 
  • #47
I haven't looked at all of the videos. but the several that I did see have 1 thing in common:
Operator error. When the chain stops due (presumably) to the anchor reaching bottom, they continue to back off the brake. When motion resumes, they are backed-off so far that they don't have a prayer of catching up. There isn't anything wrong with the equipment - it just isn't designed to recover from a situation that never should have occurred.

This seems like an idiot-proofing exercise.

A couple of things that I'd look at:

The braking mechanism shouldn't be able to back off so far.
A hydraulic speed limiter might be simple enough to prevent the 'out-of-control' situation from ever happening. Drive a pump from the capstan and friction-limit the flow / waste the energy into a water-oil HeatX. Properly executed, this arrangement might also be used as a way to measure 'deployed weight' - could be useful for determining the (apparently) confusing transition from lowering the anchor to just adding scope.

Or not.
 
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  • #48
..
Dullard said:
When the chain stops due (presumably) to the anchor reaching bottom, they continue to back off the brake. When motion resumes, they are backed-off so far that they don't have a prayer of catching up.
Agree. But it the accident is repeated so often, year after year, on different ships with different operators, that we must look at system design flaws.
Dullard said:
The braking mechanism shouldn't be able to back off so far.
I agree. In fact, I suspect that a single 360 degree turn of that wheel controls the full range from full brake to no brake.
Dullard said:
A hydraulic speed limiter might be simple enough to prevent the 'out-of-control' situation from ever happening.
Agree again. In fact that's what I'm going to explore next. I'm thinking something like a torque converter. The key to success is the shape of the brake force versus speed curve.
 
  • #50
Dullard said:
I can imagine simple, reliable solutions
The thing is mounted on the bow of ships and got permanent battering of water, salt and every harm seas can offer.
I think it's a requirement that maintenance could be done by excess amount of grease only and field repair is by hammer and wrench :wink:
 
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  • #51
Here is what I get for the chain velocity in the absence of drag, either from the capstan or fluid drag. The velocity is almost linear in time.

Dropping Anchor.JPG


I don't know if this is of interest anymore, but there it is.
 
  • #52
Rive said:
The thing is mounted on the bow of ships and got permanent battering of water, salt and every harm seas can offer.
I think it's a requirement that maintenance could be done by excess amount of grease only and field repair is by hammer and wrench
This. But I would change it slightly to say BIG hammer and BIG wrench.
 
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  • #53
Here's my thinking. I would use a water brake as a velocity limiter, or as a runaway preventer.

https://en.wikipedia.org/wiki/Water_brake

And this video,
https://en.wikipedia.org/wiki/File:Tech-Talk_Animation_on_How_Water-Brakes_Work.webm

The torque is controlled by the flow of cooling water. I would use a flyball governor to monitor capstan wheel RPM, and use the governor to control flow of water to the brake. The goal is to provide a soft limit to capstan wheel RPM; and to do it mechanically with no aux power.

The harder question is the required rating. I'm not sure how to calculate that. So partially arbitrarily, I'll choose the case of decelerating 30 feet of chain from 25 to 5 m/s velocity within 2 seconds. Here are the calculations using @erobz 's numbers

Initial V
25​
m/s
Final V
5​
m/s
Delta V
20​
m/s
Period
2​
s
Avg Acceleration
10​
m / s^2
len
30​
m
weight
269​
kg/m
total mass
8070​
kg
Initial K.E.
2521875​
Joules
Final K.E.
100875​
Joules
Power
1210500​
joules/sec
MW Power
1.2105​
MW
HP Power
1622​
Hp

I tried to find a 1.5 MW water brake on alibaba.com, but I find nothing similar. Perhaps I'm using the wrong search terms.

@erobz, @jrmichler , I'm not a M.E. Do my calculations appear correct?
Rive said:
The thing is mounted on the bow of ships and got permanent battering of water, salt and every harm seas can offer.
That's true. Ocean sailors must deal with salt and corrosion all the time. We use bronze alloys or for many objects. For example, the windlass I used to raise anchor chain on my sailboat was 100% bronze, lubricated with special water resistant grease.
 
  • #54
anorlunda said:
Here's my thinking. I would use a water brake as a velocity limiter, or as a runaway preventer.

https://en.wikipedia.org/wiki/Water_brake

And this video,
https://en.wikipedia.org/wiki/File:Tech-Talk_Animation_on_How_Water-Brakes_Work.webm

The torque is controlled by the flow of cooling water. I would use a flyball governor to monitor capstan wheel RPM, and use the governor to control flow of water to the brake. The goal is to provide a soft limit to capstan wheel RPM; and to do it mechanically with no aux power.

The harder question is the required rating. I'm not sure how to calculate that. So partially arbitrarily, I'll choose the case of decelerating 30 feet of chain from 25 to 5 m/s velocity within 2 seconds. Here are the calculations using @erobz 's numbers

Initial V
25​
m/s
Final V
5​
m/s
Delta V
20​
m/s
Period
2​
s
Avg Acceleration
10​
m / s^2
len
30​
m
weight
269​
kg/m
total mass
8070​
kg
Initial K.E.
2521875​
Joules
Final K.E.
100875​
Joules
Power
1210500​
joules/sec
MW Power
1.2105​
MW
HP Power
1622​
Hp

I tried to find a 1.5 MW water brake on alibaba.com, but I find nothing similar. Perhaps I'm using the wrong search terms.

@erobz, @jrmichler , I'm not a M.E. Do my calculations appear correct?
That's true. Ocean sailors must deal with salt and corrosion all the time. We use bronze alloys or for many objects. For example, the windlass I used to raise anchor chain on my sailboat was 100% bronze, lubricated with special water resistant grease.
I’ve got the illness that shall remain unnamed. It’s starting to wear on me. Last night my fever broke long enough I program that solution. So I’m a little more foggy than usual.

I think you need to consider the mass of the anchor as well? Also the final mass of the chain will be the initial hanging mass + the anchor+ the additional 30 m of chain at 5 m/s. You also have to change the kinetic energy of the mass that is traveling vertically inside the ship.
 
  • #55
erobz said:
I think you need to consider the mass of the anchor as well? Also the final mass of the chain will be the initial hanging mass + the anchor+ the additional 30 m of chain at 5 m/s. You also have to change the kinetic energy of the mass that is traveling vertically inside the ship.
I'm assuming that the runaway begins after the anchor touches bottom. Also assume that as soon as chain speed exceeds ship speed, the chain becomes nearly vertical, and the length of chain in motion remains constant.. But yes, I should include the K.E. of the ascending chain also; that would need about 50% more power.

Sorry to hear you're not well. Get well soon.
 
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  • #56
anorlunda said:
I'm assuming that the runaway begins after the anchor touches bottom. Also assume that as soon as chain speed exceeds ship speed, the chain becomes nearly vertical, and the length of chain in motion remains constant.. But yes, I should include the K.E. of the ascending chain also; that would need about 50% more power.

Sorry to hear you're not well. Get well soon.
So the anchor is on the bottom, but the chain hangs close to 30 m before it touches water correct?
 
  • #57
Here's how I would attack the problem of a anchoring system for a large ship:

1) Assume a worst case hanging mass. The anchor is just above the bottom of the deepest water in which the ship will be anchored.

2) Assume a maximum allowable speed of drop at that point. This value may be iterated.

3) Design a self contained passive (no electronics, operator adjustments, or electric water pumps) water brake to maintain that velocity at that load. Feel free to calculate the effect of water drag on the anchor and chain, but it's much easier to assume zero drag. That approach is most likely only slightly conservative because I think that water drag will be small compared to gravity force on the anchor and chain at any reasonable velocity.

4) Design a mechanical brake to stop that mass from that velocity in a reasonable distance. The mass and velocity are from above, the distance may be iterated. The brake should have enough braking torque to stop that mass at that speed, and enough thermal capacity to lower the full length of chain under mechanical brake control at the maximum depth at the maximum speed over ground. Design the brake operator for maximum of one or two turns from full off to full on. It should be operable by one person of average strength.

5) Design a hard stop on a spring and shock absorber arrangement to stop the chain in the case of a mechanical brake failure. The first design criteria is the free hanging mass of the chain at the maximum anchoring depth. The second design criteria is the worst case chain velocity, which may include the ship velocity over ground. The anchor will be on the bottom at this point. You may or may not want to consider the case of a powerless ship driven by wind and/or current and the anchor not slipping. The spring and shock absorber arrangement may activate if the brake is applied too hard, so it should be self resetting.

6) Design the system weak link. The existing weak link is the attachment of the chain to the ship. Remember that it's better to lose an anchor and chain than to pull the bow of the ship off.

This system should allow both fast drops and controlled drops, and allows for operator error on the brake. This system will allow manual control of drops with a failed water brake. It will allow anchoring with a mechanical brake that failed in the open (unbraked) position by letting the chain run all the way out, then winching back to the desired length.
 
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  • #58
hutchphd said:
Here's a nice very short compendium on magnetic brakes:
I considered that. These are incredible things - they can stop very, very, very heavy objects on a dime. However, I think in principle they suffer from the same problem as mechanical brakes - what do you do with the energy?
 
  • #59
jrmichler said:
6) Design the system weak link. The existing weak link is the attachment of the chain to the ship. Remember that it's better to lose an anchor and chain than to pull the bow of the ship off.
A weakest chain link is supposed to be built into the chain near the end.
The chain can be manually emergency separated from the hull - ie weather deteriorates to the anchor drag situation
 
  • #60
anorlunda said:
I'm assuming that the runaway begins after the anchor touches bottom. Also assume that as soon as chain speed exceeds ship speed, the chain becomes nearly vertical, and the length of chain in motion remains constant.. But yes, I should include the K.E. of the ascending chain also; that would need about 50% more power.
Ship speed should be zero when dropping anchor.
 

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