[HN Gopher] Seventy versus One Hundred
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       Seventy versus One Hundred
        
       Author : ColinWright
       Score  : 44 points
       Date   : 2023-12-27 11:14 UTC (1 days ago)
        
 (HTM) web link (www.solipsys.co.uk)
 (TXT) w3m dump (www.solipsys.co.uk)
        
       | didgeoridoo wrote:
       | Nerd snipe alert. Do not open this if you're just getting into
       | bed.
        
         | cheschire wrote:
         | https://www.explainxkcd.com/wiki/index.php/356:_Nerd_Sniping
        
       | dylan604 wrote:
       | "(keep scrolling ...) "
       | 
       | ...
       | 
       | "(was that far enough?) "
       | 
       | oh man, i was hoping this was going to be one of those tricks of
       | no matter what your window size was, this would always be just
       | below the fold with CSS. i just got lucky for it to line up.
       | after trying it again with a smaller window, it was just in the
       | scroll. =(
       | 
       | then again, looking at the site's layout, it does not really
       | suggest heavy use of CSS. at. all.
        
       | dmoy wrote:
       | TL;DR v^2 is bad for your health in a car crash
       | 
       | (But probably read it because it's really short)
        
         | dylan604 wrote:
         | yeah, if we need a TL;DR version of that...well, boy, I just
         | don't know
        
       | krukah wrote:
       | > Let's assume that the brakes are working at their limit, and as
       | they do so, they are shedding energy at a maximum rate that
       | doesn't change. The cars are identical, so they are both shedding
       | energy at the same rate per unit distance.
       | 
       | Interesting (and I think very reasonable) first-order assumption.
       | Maybe to second-order, the calculation could assume the braking
       | force is proportional to velocity, which I think is roughly true
       | of friction generally, but is also harder to model.
        
         | bell-cot wrote:
         | IANAE (...not an engineer), but "braking force is proportional
         | to velocity" is not how brakes, or friction, work.
        
           | purpleflame1257 wrote:
           | No, but it is how first-order atmospheric drag is modeled,
           | which may be what confused the GP comment.
        
         | Karellen wrote:
         | > > they are both shedding energy at the same rate per unit
         | distance.
         | 
         | > Interesting (and I think very reasonable) first-order
         | assumption.
         | 
         | Really? That triggered alarm bells in my head _immediately_. I
         | mean, it might be true, but I 'd need to do the math to figure
         | it out one way or another.
         | 
         | > the calculation could assume the braking force is
         | proportional to velocity, which I think is roughly true of
         | friction generally
         | 
         | Again, not my intuition at all. I'd have gone with the braking
         | force being constant at non-zero velocity. (And force is
         | variable up to the limit of static friction when at zero
         | velocity.)
        
       | lmm wrote:
       | I assumed constant deceleration. Then u = sqrt(v^2 - 4as), a and
       | s are constant so = sqrt(v^2-70^2) = approximately 70mph.
        
         | FabHK wrote:
         | That's the same assumption as the (first) article makes.
        
           | lmm wrote:
           | It talks about shedding energy at a constant rate per
           | distance. Which, sure, ends up giving the same result, but
           | it's a much weirder starting assumption, IMO.
        
             | Ma8ee wrote:
             | I thought it was a quite natural assumption, considering
             | the same brake friction force and that the work done by
             | that is the force times the distance. (W = Fs).
        
       | tempestn wrote:
       | Cars can generally decelerate at a roughly constant rate of
       | acceleration, based on the friction between tires and ground.
       | Given the cars are identical, you can therefore define braking
       | acceleration (deceleration) a, which is equal to both 70/t1 and
       | (100-v)/t2, where v is the final velocity we're solving for.
       | 
       | We also know that the average velocity for each car equals the
       | distance travelled over time elapsed, where the distance is equal
       | for both cars, but the time isn't. So, 70/2 = d/t1 and (100+v)/2
       | = d/t2.
       | 
       | Can then solve these equations for v ~= 71.4
       | 
       | The gotcha is that it's much easier to solve if you take both
       | distance and time as constant for both cars, but that would be a
       | mistake.
       | 
       | Of course you could get even more meta with it. Since the faster
       | car is going to reach the obstacle first and smash into it, it
       | probably won't be in the same position when the slower car
       | reaches it either!
        
         | neerajsi wrote:
         | Yeah, I also got 71.4 according to the same logic, but I can
         | buy the argument in the follow on article that the amount of
         | energy dissipated per unit time is what's constant.
        
           | tempestn wrote:
           | Why? No production car is brake limited; slam on the brakes
           | in any car and you'll go into (and stay in) ABS, meaning
           | you're at the limit of tire grip, and therefore at roughly
           | constant deceleration. Where would energy dissipation come
           | into the picture? The energy is being dissipated by the
           | brakes, not the tires, and they're not the limiting factor.
        
             | eschneider wrote:
             | Not true. Brakes need time to dump heat. With repeated hard
             | braking it's not too hard to overwhelm the brakes on most
             | cars.
        
               | tempestn wrote:
               | But the scenario we're talking about here isn't repeated
               | hard braking.
        
             | klodolph wrote:
             | There is a different, clever way to analyze the problem
             | thinking about energy and work.
             | 
             | Work is by definition (work) = (force) x (distance), or the
             | same thing expressed as an integral.
             | 
             | Distance is the same, that's a parameter of the problem. If
             | we say that the brakes apply constant deceleration, then
             | that implies that the force is the same, between both cars.
             | Then the amount of energy shed by both cars is the same
             | before they reach the barrier. (We don't need to use the
             | integral definition for work here, because force is a
             | constant.)
             | 
             | This explains why the people who assumed that both cars
             | dump the same amount of energy arrived at the same result,
             | even though some of the people in this thread appear to be
             | using faulty reasoning.
        
               | tempestn wrote:
               | Ah, of course, you're right. Thanks for pointing that
               | out! I didn't really think about it at the time, but the
               | equation you end up with if you use the acceleration
               | approach results in a v^2, which makes sense when you
               | consider that the equal energy dissipation approach is
               | equivalent.
        
       | Ntrails wrote:
       | I mean this also misses the fact that if they _see_ the obstacle
       | at the exact same distance + time (a sensible assumption to
       | compare) by the time they hit the breaks a significant difference
       | in distance has already been generated.
       | 
       | Stopping distances are part of the theory test in the UK, albeit
       | with nonsense values. The frustrating part for me is how they
       | completely ignore differences due to vehicles and gloss over road
       | conditions.
        
         | HarHarVeryFunny wrote:
         | Even tire brand/model (and wear) can have a significant effect
         | on braking distance.
        
       | HarHarVeryFunny wrote:
       | I don't know how valid the "brakes shedding energy at same rate
       | per unit distance" is, but other sources confirm how massively
       | braking distance increases with speed.
       | 
       | For example, from here:
       | 
       | https://www.automotive-fleet.com/driver-care/239402/driver-c...
       | 
       | At 50 mph braking distance is 125 ft.
       | 
       | At 60 mph it's 245 ft
       | 
       | At 80 mph it's 439 ft
       | 
       | Now, when you consider the emergency circumstances where you
       | might be flooring the brakes, this is not good ...
       | 
       | e.g.
       | 
       | A deer or child runs out in front of you, so close that emergency
       | braking is called for .. how far away are they going to be from
       | you ?
       | 
       | Or, say the car in front of you on highway slams on their brakes,
       | and they were travelling at 50mph, with you approaching at 60mph.
       | Unless you are at least 120 ft behind them (vs the typical
       | highway following distance of a few car lengths), you are going
       | to be in a bad head-on collision.
        
         | zamadatix wrote:
         | > At 50 mph braking distance is 125 ft.
         | 
         | > At 60 mph it's 245 ft
         | 
         | > At 80 mph it's 439 ft
         | 
         | It looks like you're jumping between columns and sometimes
         | transposing rows here. 125' @ 50 mph is from the raw braking
         | distance column, 245' is from the same column but for 70 mph
         | rather than 60 mph, and 439' @ 80 mph is from the overall
         | stopping distance column. I'm not pointing this out just to
         | nit, rather because:
         | 
         | > say the car in front of you on highway slams on their brakes,
         | and they were travelling at 50mph, with you approaching at
         | 60mph. Unless you are at least 120 ft behind them (vs the
         | typical highway following distance of a few car lengths), you
         | are going to be in a bad head-on collision.
         | 
         | You've concluded nearly twice the stopping footage as the table
         | actually says and, as is more directly said in the last column,
         | it's really roughly a 4 car braking length difference between
         | the two speeds (including reaction time).
        
         | adewinter wrote:
         | Kinetic energy scales with velocity squared (0.5 _m_ v^2), so
         | this result makes sense. Brakes dissipate constant energy, but
         | the amount of energy it needs to disapate is going up much
         | faster.
        
         | margalabargala wrote:
         | > I don't know how valid the "brakes shedding energy at same
         | rate per unit distance" is
         | 
         | From the follow-up post, the author gives a justification for
         | that.
         | 
         | > the force applied by the brake pads on the brake disc is
         | going to be roughly constant, and so the work done, which in
         | this case is the energy shed, is the force times the distance
         | over which the force is applied.
         | 
         | There will of course be confounding factors like temperature,
         | etc. But it's probably pretty close.
        
       | beefman wrote:
       | Ignoring the obstacle:
       | 
       | * It may be reasonable to assume the brakes produce the same
       | force on both cars. With both cars weighing the same, this
       | produces the same acceleration. Then the speeds decrease at the
       | same rate, which means the faster car is going 100 - 70 = 30 kph
       | when the slower car stops.
       | 
       | * The faster car must dissipate more energy to do this. We may
       | assume that braking is limited by heat dissipation and that the
       | brakes shed energy at the same rate. Then the answer is
       | sqrt(100^2 - 70^2) ~ 71 kph.
       | 
       | Adding the obstacle:
       | 
       | * As noted in the text, brakes don't shed energy at the "same
       | rate per unit distance". So the faster car hits the obstacle
       | first, at greater speeds than above in each case. We aren't given
       | the information required to calculate the stopping time or
       | distance of the slower car, so the problem is underspecified.
        
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       (page generated 2023-12-28 23:00 UTC)