What distance will be covered before coming to stop?

In summary, the distance covered before coming to a stop is determined by factors such as initial speed, deceleration rate, and the conditions affecting stopping (like friction). The formula to calculate this distance is derived from physics, specifically using equations of motion, and can be influenced by the weight of the vehicle, road conditions, and braking efficiency.
  • #1
chwala
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Homework Statement
A train braking with constant deceleration covers ##1## km in ##20s##, and a second kilometre in ##30s##. Find the deceleration. What further distance will it cover before coming to a stop, and how long will this take?
Relevant Equations
Mechanics
1717370611427.png


Phew; back n forth on this anyway, my lines

...

##v_{1} = \dfrac{1000}{20} = 50## m/s in the first ##10## seconds.


##v_{2} = \dfrac{1000}{30} = \dfrac{100}{3} ##m/s in the first ##35## seconds.

where ##v_1## and ##v_2## are the respective velocities in ##10s## and ##35s## respectively.

Thus,

##a = \dfrac{33.3333 - 50}{35-10} = -\dfrac{2}{3}m/s^2##.

Therefore deceleration is equal to ##\dfrac{2}{3} m/s^2= 0.666m/s^2##.

For next part,

##v=u+at##

##v_{3}= 33.333+(-0.666×15)##

##v_{3} = 23.3333## m/s

using ##v^2 =u^2 +2as##

##0 = 23.333 + (2×-0.666×s)##

##544.3 = 1.333s##

##s = 408.3m## correct to one decimal place.

Finally,

Using ##v= u+at##

##0 = 23.333+ (-0.666t)##

##23.333= 0.66t##

##t =35## seconds

There could be a much better approach hence my post. Cheers.
 
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  • #2
chwala said:
There could be a much better approach hence my post.
There is. I can't read the problem, but I can tell you that plugging in numbers is the last step, not the first.
 
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  • #3
Vanadium 50 said:
There is. I can't read the problem, but I can tell you that plugging in numbers is the last step, not the first.
I re-typed the question.
 
  • #4
chwala said:
##v_{1} = \dfrac{1000}{20} = 50## m/s in the first ##10## seconds.
I agree.
chwala said:
##v_{2} = \dfrac{1000}{30} = \dfrac{100}{3} ##m/s in the first ##35## seconds.
Where did 35 come from?
Why do you care about the average velocity for the first 35 seconds?
Did you actually compute the average velocity for the first 35 seconds?
Out of purely idle curiosity, what would be the average velocity over the second interval?
 
  • #5
jbriggs444 said:
I agree.

Where did 35 come from?
Why do you care about the average velocity for the first 35 seconds?
Did you actually compute the average velocity for the first 35 seconds?
Out of purely idle curiosity, what would be the average velocity over the second interval?

For an object moving with constant acceleration or deceleration over a period of time, then it is common knowledge that these quantities are the same;
  • average velocity
  • velocity when half the time has passed
  • mean of the initial and final velocities

Where did 35 come from?

From ##t = 20 + \dfrac{30}{2} s##.


Did you actually compute the average velocity for the first 35 seconds?

In the last ##30## seconds, the average velocity is ##\dfrac{1000}{30} m/s##, so this is the velocity after ##(20 +15) = 35## seconds, from this i am able to determine the rate of deceleration as indicated.
 
  • #6
chwala said:
In the last ##30## seconds, the average velocity is ##\dfrac{1000}{30} m/s##, so this is the velocity after ##(20 +15) = 35## seconds, from this i am able to determine the rate of deceleration as indicated.
Ahhh, there seems to be a language difficulty.

You'd originally written:
chwala said:
##v_{1} = \dfrac{1000}{20} = 50## m/s in the first ##10## seconds.
This is phrased unfortunately. I would have said instead:

The average velocity is 50 m/s over the first 20 seconds.

Given constant acceleration, it follows that the instantaneous velocity is 50 m/s at the 10 second mark".

Similarly:
chwala said:
##v_{2} = \dfrac{1000}{30} = \dfrac{100}{3} ##m/s in the first ##35## seconds.
Where I would have said:

The average velocity is ##\frac{1000}{30} \text{ m/s}## over the next 30 seconds.

Given constant acceleration, it follows that the instantaneous velocity is ##\frac{1000}{30} \text{ m/s}## at the 35 second mark.
 
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  • #7
jbriggs444 said:
Ahhh, there seems to be a language difficulty.

You'd originally written:

This is phrased unfortunately. I would have said instead:

The average velocity is 50 m/s over the first 20 seconds.

Given constant acceleration, it follows that the instantaneous velocity is 50 m/s at the 10 second mark".

Similarly:

Where I would have said:

The average velocity is ##\frac{1000}{30} \text{ m/s}## over the next 30 seconds.

Given constant acceleration, it follows that the instantaneous velocity is ##\frac{1000}{30} \text{ m/s}## at the 35 second mark.
Were you having a different approach where ##35## is not going to be considered as part of working?
 
  • #8
chwala said:
Were you having a different approach where ##35## is not going to be considered as part of working?
No. I was merely concerned that an average velocity over a period of 35 seconds would have nothing to do with the solution.

Your original statements appeared to claim an average velocity of ##\frac{1000}{30} \text{ m/s}## over the interval from ##t=0## to ##t=35##.

Yes, the computations you performed match the ones would have performed. The concern was with the explanations [or lack thereof] for those computations.

The advice from @Vanadium 50 in #2 is apt: Explanations first, computations after.
 
  • #9
The formal approach recognizes that one is given two pairs of positions and clock times. Assuming that ##t=0## is when the train starts braking, one has
##(x_1,t_1)=(1~{\text{km}},20~{\text{s}})##
##(x_2,t_2)=(2~{\text{km}},50~{\text{s}})##

Then one writes the position SUVAT equation twice to get a system of two equations and two unknowns
##x_1=v_0t_1+\frac{1}{2}at_1^2##
##x_2=v_0t_2+\frac{1}{2}at_2^2##
The unknowns are the initial velocity ##v_0## and acceleration ##a##.

I leave the rest as an exercise to the student.
Hint: Divide the first equation by ##t_1##, the second equation by ##t_2## and subtract.

Substitute numbers at the very end.
 
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  • #10
kuruman said:
The formal approach recognizes that one is given two pairs of positions and clock times. Assuming that ##t=0## is when the train starts braking, one has
##(x_1,t_1)=(1~{\text{km}},20~{\text{s}})##
##(x_2,t_2)=(2~{\text{km}},50~{\text{s}})##

Then one writes the position SUVAT equation twice to get a system of two equations and two unknowns
##x_1=v_0t_1+\frac{1}{2}at_1^2##
##x_2=v_0t_2+\frac{1}{2}at_2^2##
The unknowns are the initial velocity ##v_0## and acceleration ##a##.

I leave the rest as an exercise to the student.
Hint: Divide the first equation by ##t_1##, the second equation by ##t_2## and subtract.

Substitute numbers at the very end.
...
I was able to realize,

##2000 = 40v_0 +400a## and
##4000 = 100v_0 +2500a##

Solving for the unknown, i can see that ##a= -\dfrac{2}{3} m/s^2##

Now to my next question, for the unknown ##v_0## i have ##v_0 = 56.7m/s##. This is the initial velocity at what point? before deceleration?
 
  • #11
chwala said:
...
for the unknown ##v_0## i have ##v_0 = 56.7m/s##. This is the initial velocity at what point? before deceleration?
Yes.

For an ad hoc approach, it slowed from an average of 50m/s over 20s to 33.33m/s over 30s. Those average speeds would have been the instantaneous speeds in the centres of those intervals, so it slowed from 50 to 33.33 in 20/2+30/2=25 seconds.
 
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  • #12
chwala said:
...
I was able to realize,

##2000 = 40v_0 +400a## and
##4000 = 100v_0 +2500a##

Solving for the unknown, i can see that ##a= -\dfrac{2}{3} m/s^2##

Now to my next question, for the unknown ##v_0## i have ##v_0 = 56.7m/s##. This is the initial velocity at what point? before deceleration?
You missed my point in post #9. The idea is not to susbstitute numbers in the middle of the solution. Here is what I had in mind.
Divide each equation by the times
$$\begin{align} & x_2/t_2=v_0+\frac{1}{2}at_2 \nonumber \\& x_1/t_1=v_0+\frac{1}{2}a t_1 \nonumber \end{align}$$Subtract bottom equation from top and solve for the acceleration $$\begin{align}
& x_2/t_2-x_1/t_1=\frac{1}{2}a(t_2 -t_1) \nonumber \\
&a=\frac{ x_2/t_2-x_1/t_1}{\frac{(t_2 -t_1)}{2}}. \nonumber
\end{align}$$This symbolic expression shows what's going on here. The last equation is a straightforward application of ##a=\Delta v/\Delta t## where ##v## is the instantaneous velocity. Note that the average velocity over interval ##t_2## is ##\bar v_2=x_2/t_2## and is equal to the instantaneous velocity ##v_2## at time ##t'_2=\frac{1}{2}t_2##. Likewise, the average velocity over interval ##t_1## is ##\bar v_1=x_1/t_1## and is equal to the instantaneous velocity ##v_1## at time ##t'_1=\frac{1}{2}t_1##. Thus the acceleration is $$a=\frac{v_2-v_1}{t'_2-t'_1}=\frac{ x_2/t_2-x_1/t_1}{\frac{(t_2 -t_1)}{2}}.$$My point is the same as @Vanadium 50 raised. You don't get a deeper understanding of what's going unless you substitute numbers at the very end. You could have written the expression for the acceleration immediately by putting together these three ideas when an object moves under constant acceleration
  1. The average velocity is the position change over the time interval of the change.
  2. The instantaneous velocity is equal to the average velocity at half the time interval of the change.
  3. The acceleration is equal to the change of instantaneous velocity over the time interval of the change.
 
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  • #13
chwala said:
This is the initial velocity at what point? before deceleration?
What do you think? What does the expression for the instantaneous velocity look like?
 

FAQ: What distance will be covered before coming to stop?

1. What factors affect the distance covered before coming to a stop?

The distance covered before coming to a stop is influenced by several factors, including the initial speed of the object, the friction between the object and the surface it is moving on, the mass of the object, and any external forces acting on it (such as air resistance or braking force in vehicles).

2. How can I calculate the stopping distance for a vehicle?

The stopping distance can be calculated using the formula: Stopping Distance = (Initial Speed)^2 / (2 × Deceleration). The deceleration can be determined from the friction coefficient between the tires and the road surface, as well as any braking force applied.

3. Does the type of surface affect the stopping distance?

Yes, the type of surface significantly affects the stopping distance. For example, a rough surface (like gravel) will provide more friction and result in a shorter stopping distance compared to a smooth surface (like ice or wet pavement), which offers less friction.

4. How does speed impact the stopping distance?

The stopping distance increases with the square of the speed. This means that if the speed doubles, the stopping distance increases by a factor of four, making it crucial for drivers to maintain safe speeds to ensure they can stop in time.

5. Can external factors like weather conditions affect stopping distance?

Yes, weather conditions such as rain, snow, or ice can greatly impact stopping distance. Wet or icy roads reduce tire traction, leading to longer stopping distances. Drivers should adjust their speed and following distances in adverse weather conditions to account for this increased stopping distance.

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