A new take on a relative velocity problem

Click For Summary
The discussion centers on solving a relative velocity problem involving a bullet and a balloon, where the goal is to determine the minimum speed of the bullet required to pop the balloon. A peer attempted to solve the problem using four different equations, but only the second equation yielded a minimum value for the bullet's speed. The second equation effectively incorporates the balloon's height and speed, while the others do not provide essential information for the specific scenario. The conversation highlights the importance of understanding the physical context behind the equations used and emphasizes that the minimum speed is crucial for ensuring the bullet reaches the balloon at the right moment. Overall, the thread illustrates the complexities of applying mathematical concepts to real-world physics problems.
  • #31
PeroK said:
One of your problems here is a sloppiness in notation that many books follow. We shouldn't really use ##t## for both the continuous variable of time and the fixed time of the collision. For this we should use ##t_0## or ##t_1## or ##T##.

An equation like ##v = u + at## is just a general equation for the velocity of the bullet. It carries no specific information about this problem.

The second equation, however, is an equation for ##T## the time to hit the balloon:
$$u = (25 \ m/s)T + \frac 1 2 gT + \frac{ 125 \ m}{T}$$That equation contains all the information about the problem: in particular the initial height and speed of the balloon. We would normally think of ##T## being a function of ##u##: choose an initial speed, ##u##, and (assuming it's large enough) we get some time ##T## of impact.

Turning this round, we can look at choosing an impact time ##T## and, assuming its short enough, we can find the initial speed that gives that impact time.

Then we notice that minimising the speed with respect to possible impact times solves the problem.

Your problem is that you applied some mathematics (function minimisation) without understanding how the function related to your physical problem. And I had to piece it all together for you!
But t here(v=u+at) is still the same time taken for the bullet to reach the balloon,right? Also could you mention what information this equation is missing?
 
  • Like
Likes Shreya
Physics news on Phys.org
  • #32
PeroK said:
Let's analyse your last attempt. From ##v^2 - u^2 = 2as## you got:
$$u^2 = v^2 +2g(h_0 + v_b t)$$But, then you plugged in ##v = 25 \ m/s##, which destroys the minimisation approach - as this ##v## is a specific solution. Instead, you need to use ##v = u -gt## to get:
$$u^2 = u^2 -2ugt + g^2t^2 +2g(h_0 + v_bt)$$Hence:
$$2ugt = g^2t^2 + 2gv_bt + 2gh_0$$And:
$$u = \frac 1 2 gt + v_b + \frac{h_0}{t}$$Which is the same equation we got above. Again, it might be better to use ##T## to indicate the time of impact.
Why does it work only when we keep v as u - gt ?
 
  • #33
Differentiate it said:
But t here(v=u+at) is still the same time taken for the bullet to reach the balloon,right? Also could you mention what information this equation is missing?
That equation applies to the bullet regardless of what the balloon is doing.
 
  • Informative
Likes Shreya
  • #34
PeroK said:
That equation applies to the bullet regardless of what the balloon is doing.
Whoops, my bad, that was a silly question 😅
What about the other question though?
 
  • #35
Differentiate it said:
Why does it work only when we keep v as u - gt ?
Because ##v = 25 \ m/s## implies the specific solution and determines ##u## and ##t##. These are then no longer continuous variables. If ##v = 25 m/s##, then ##u = 75 \ m/s## and ##t = 5 \ s## and there is no function to differentiate.
 
  • Informative
Likes Shreya
  • #36
PeroK said:
Because v=25 m/s implies the specific solution and determines u and t. These are then no longer continuous variables. If v=25m/s, then u=75 m/s and t=5 s and there is no function to differentiate.
Awesome! Does that mean that the equations we get in 3 & 4 doesn't describe the range of ##u##s and the corresponding ##t##s we can get, but only a specific situation.
Another Silly Question - then why do we still get a function (not a number)? And doesn't the lower values of u from 3 & 4 satisfy the conditions?
 
  • #37
neilparker62 said:
I did not contribute much other than trying to ensure balloon popping! But thanks for including me in the "credits" list all the same.!

Delta2 said:
I didnt contribute much either, I think 95% of the thanks should go to Perok, Andrewkirk and Kuruman
For a student who is self learning physics with no conventional teacher & only access to internet, and who has spent more than 3 hrs on this problem myself with no progress, anybody who has contributed is godlike
 
  • Like
Likes Lnewqban, neilparker62 and Delta2
  • #38
PeroK said:
Because ##v = 25 \ m/s## implies the specific solution and determines ##u## and ##t##. These are then no longer continuous variables. If ##v = 25 m/s##, then ##u = 75 \ m/s## and ##t = 5 \ s## and there is no function to differentiate.
But u and t are both unknown. u can be any value and t can be any value too, right?
 
  • #39
PeroK said:
That equation applies to the bullet regardless of what the balloon is doing.
Hm, but how does s = ut + (1/2)at^2 take the balloon's motion into account? s is the displacement of the bullet(displacement of the balloon from when the bullet is fired to when it hits the balloon is just 25t), u is the bullets initial velocity, and t is the time taken to hit the balloon
 
  • #40
Differentiate it said:
Hm, but how does s = ut + (1/2)at^2 take the balloon's motion into account? s is the displacement of the bullet(displacement of the balloon from when the bullet is fired to when it hits the balloon is just 25t), u is the bullets initial velocity, and t is the time taken to hit the
##v=u+at## just takes into account the fact that the bullet experiences deceleration and will have a final Velocity of ##v## later. It is too general and doesn't take into account the distance the bullet has to cover to pop the balloon (or anything regarding the situation), while ##s=ut+\frac{1}{2}at²## states that the bullet has to cover the required distance while experiencing deceleration.
Note that ##v=u+at## can be used for any object moving up against gravity and reaches the said ##v## - it doesn't have what we are looking for ie the bullet has to pop the balloon
 
  • Like
Likes Differentiate it
  • #41
Shreya said:
Awesome! Does that mean that the equations we get in 3 & 4 doesn't describe the range of ##u##s and the corresponding ##t##s we can get, but only a specific situation.
Another Silly Question - then why do we still get a function (not a number)? And doesn't the lower values of u from 3 & 4 satisfy the conditions?
Essentially you do get a number (really a quantity, as we have units involved). There's a difference between a fixed, as yet uncalculated quantity and a variable. To take a simple example.

We start with the simple equation relating displacement, constant velocity and time:
$$s = vt$$In general, all of these quantities may be variables. Note that there is a subtle difference between ##v##, which is an unknown, and ##s## and ##t## which are continuous variables.

In a single experiment, ##v## would be some fixed quantity throughout the experiment, while ##t## and ##s## vary.

If we consider varying ##v##, then we are considering many different experiments. This is the technique you tried to use for this problem. This is a valid approach, but you must be aware of what you are doing.

If we want to hit a target at a distance of ##10 \ m## then the speed and time are related by:
$$vT = 10 \ $$Which gives ##v## as a function of ##T## and vice versa. We can plot a graph of ##v## against ##T##. Note that I've been careful to use ##T## here to indicate that we have a fixed but unknown time ##T##. In any experiment we have a single ##v## and a single value for ##T##. This ##T## is not the same as the continuous variable ##t## that represents the passage of time.

In this case, there is no minimum of maximum, but we can still draw a graph of the function ##v(T) = \frac{10 \ m}{T}## or ##T(v) = \frac{10 \ m}{v}##.

Note that this is a function that represents many different experiments, with all the possible values of ##v##. In any given experiment, ##v## and ##T## are fixed (even if unknown) quantities.

Finally, if we assume that ## v = 5 \ m/s##, say, then we no longer have a function and ##T## must be ##2 \ s##. In this simple case, as soon as we choose either ##v## or ##T## then the function collapses to a single point on the graph. This is what happened above when you chose ##v = \ 25 m\s## as the final speed. You had then specified enough data to collapse the function relating ##u## and ##T## to a single point on the graph (##u = 75 \ m/s## and ##T = 5 \ s##). Even if you still had to calculate these numbers.

In particular, you no longer had a function ##u(T)## to do calculus on.
 
  • Like
  • Informative
Likes Lnewqban and Shreya
  • #42
Differentiate it said:
But u and t are both unknown. u can be any value and t can be any value too, right?
No. Once you specify ##v = 25 \ m/s##, this fixes the values of ##u## and ##t##, even if you still have to calculate them.
 
  • Like
Likes Shreya
  • #43
Differentiate it said:
Hm, but how does s = ut + (1/2)at^2 take the balloon's motion into account?
Because you combine that equation for the bullet with the simultaneous equation for the motion of the balloon. If we do this formally, we have:
$$s = ut - \frac 1 2 gt^2$$and$$s_b = h_0 + v_bt$$And we set ##s = s_b## to get the equation relating the initial speed of the bullet and the time of impact:
$$uT - \frac 1 2 gT^2 = h_0 + v_bT$$This equation then contains all the information relating the initial speed of the bullet with the time of impact. Note that ##h_0## and ##v_b## are fixed quantities and not variables in this case.

Note that ##u, T## are variables here representing many different physical experiments. And we have a function relating them.

But, if we specify additionally the final speed of the bullet when it hits the balloon, then there is only one possible initial speed and one possible time. This is because if we fix ##v = u -gT = 25 \ m/s##, then we have another equation relating ##u## and ##T##. And the equation above reduces to:
$$u = 75 \ m/s \ \ \text{or} \ \ T = 5 \ s$$
 
Last edited:
  • Like
Likes Shreya
  • #44
Essentially, the last 2 equations specify the final Velocity, thereby fixing ##u## & ##T##, even though they are unknown, they refer to one specific experiment. The graph has collapsed to a single point and is no longer differentiable. The value of ##u## still has to be calculated using simultaneous equations but has already been fixed on specifying ##v##. But on using ##u-gT## for ##v## I still refer to multiple experiments and multiple values of ##u## and ##t## and therefore I can use function minimization.
Please correct me if something is wrong
 
  • Like
Likes PeroK
  • #45
Shreya said:
Essentially, the last 2 equations specify the final Velocity, thereby fixing ##u## & ##T##, even though they are unknown, they refer to one specific experiment. The graph has collapsed to a single point and is no longer differentiable. The value of ##u## still has to be calculated using simultaneous equations but has already been fixed on specifying ##v##. But on using ##u-gT## for ##v## I still refer to multiple experiments and multiple values of ##u## and ##t## and therefore I can use function minimization.
Please correct me if something is wrong
Isn't there multiple values for u and t even though we fix v as 25?
We can still represent u as a function of t, it doesn't collapse it to a point
 
  • #46
Shreya said:
Essentially, the last 2 equations specify the final Velocity, thereby fixing ##u## & ##T##, even though they are unknown, they refer to one specific experiment. The graph has collapsed to a single point and is no longer differentiable. The value of ##u## still has to be calculated using simultaneous equations but has already been fixed on specifying ##v##. But on using ##u-gT## for ##v## I still refer to multiple experiments and multiple values of ##u## and ##t## and therefore I can use function minimization.
Please correct me if something is wrong
Isn't there multiple values for u and t even though we fix v as 25?
We can still represent u as a function of t, it doesn't collapse
 
  • #47
Differentiate it said:
Isn't there multiple values for u and t even though we fix v as 25?
We can still represent u as a function of t, it doesn't collapse it to a point
Yes, but let's not forget that the distance the balloon has to travel is fixed - and on fixing the final Velocity - the graph collapses to a single point which is (5,75)
Please correct me if I'm wrong
 
  • #48
Differentiate it said:
Isn't there multiple values for u and t even though we fix v as 25?
We can still represent u as a function of t, it doesn't collapse
No, it's fully constrained by specifying that it impacts the balloon at ##25 \ m/s##. There is only one physical solution for the initial speed (##u = 75 \ m/s##) and only one solution to the simultaneous equations.

You may be confusing the trajectory of the bullet, defined by ##s = ut - \frac 1 2 gt^2## and the relationship between the initial speed and the time at which the bullet hits the balloon: ##u(T)##.

It's critical to use different symbols (##t## and ##T##) for these concepts. Using the same symbol ##t## for both only works as long as you keep the concepts separate in your mind.
 
Last edited:
  • Like
Likes Shreya
  • #49
PeroK said:
No, it's fully constrained by specifying that it impacts the balloon at ##25 \ m/s##. There is only one physical solution for the initial speed (##u = 75 \ m/s##) and only one solution to the simultaneous equations.

You may be confusing the trajectory of the bullet, defined by ##s = ut - \frac 1 2 gt^2## and the relationship between the initial speed and the time at which the bullet hits the balloon: ##u(T)##.

It's critical to use different symbols (##t## and ##T##) for these concepts. Using the same symbol ##t## for both only works as long as you keep the concepts separate in your mind.
I don't understand...
Also, does a function have no minima if there's 2(or maybe more) minimum values? Because here u is minimum, s and t are maximum. Whereas v is minimum. But when you substitute in say u -gt for v, instead of to minimum variables u and v, you have only u.
And the function u(t) has a minima
If yes, why?
It's probably wrong, but could you explain it more? I don't get how u is fixed to 75 if I set v = 25.
 
  • #50
Differentiate it said:
I don't understand...
Also, does a function have no minima if there's 2(or maybe more) minimum values? Because here u is minimum, s and t are maximum. Whereas v is minimum. But when you substitute in say u -gt for v, instead of to minimum variables u and v, you have only u.
And the function u(t) has a minima
If yes, why?
It's probably wrong, but could you explain it more? I don't get how u is fixed to 75 if I set v = 25.
I can't explain it more until you start using ##T## when you mean the time of impact for a given ##u##.
 
  • #51
PeroK said:
I can't explain it more until you start using ##T## when you mean the time of impact for a given ##u##
Uhhh, just use T and explain..?
 
  • #52
Differentiate it said:
Uhhh, just use T and explain..?
I need to see an attempt on your part to understand the difference between the continuous time coordinate ##t## and the time of impact ##T##.
 
  • Like
Likes Shreya
  • #53
PeroK said:
I need to see an attempt on your part to understand the difference between the continuous time coordinate ##t## and the time of impact ##T##.
could you at least answer the question I made a posts ago? I know its probably wrong, but just want to know if its correct, also I don't understand how u and t both are fixed when we fix v
 
  • #54
PeroK said:
I need to see an attempt on your part to understand the difference between the continuous time coordinate t and the time of impact T
I think he just wants you to re-ask your question in post #49 by replacing ##t## with ##T## wherever applicable. Example, You have - "##t## are maximum" ##\rightarrow## ##T## are maximum.
And In post #53, you said "##u## and ##t##" are fixed, while you should have said ##u## and ##T## are fixed. (Cause any choice of ##u## or ##v## doesn't fix the independent ##t## but it does fix ##T##)
It may not seem like a big difference - but it is. ##t## is the independent continuous variable as @PeroK mentioned while ##T## is the impact time.
Moreover you are minimizing ##u(T)## not ##u(t)## & the graphs given were of ##u(T)##. Also note that ##u## doesn't depend on ##t## but It does on ##T##
It's my fault - because I used the wrong notation first and caused this confusion 😕.
 
Last edited:
  • Love
Likes PeroK
  • #55
Delta2 said:
at least 90km/h but I don't know something doesn't look 100% rigorous with this, I found the approach described in post #2 more rigorous than the approach of post #4.

However post #4 is what we call a "clever shortcut".
The approach in post #4 is perfectly rigorous. Changing frames is not fishy in any way. The speed vs height follows from the SUVAT equations with final speed set to zero at the limiting case.
 
  • Like
Likes PeroK and Shreya
  • #56
Orodruin said:
Changing frames is not fishy in any way
Yes ok, I guess it is just me. Never feel comfortable when we use multiple reference frame in a single problem. That's also one reason I can't study relativity (the other main reason , not knowing tensor calculus lol).
 
  • Like
Likes Shreya
  • #57
Delta2 said:
Yes ok, I guess it is just me. Never feel comfortable when we use multiple reference frame in a single problem. That's also one reason I can't study relativity
This piques my interest. Where is the limit? Are you fine with using different Cartesian coordinate systems in geometry? What about using spherical coordinates?

Delta2 said:
the other main reason , not knowing tensor calculus lol
I know a good book … 😁
 
  • Like
Likes Shreya
  • #58
Orodruin said:
This piques my interest. Where is the limit? Are you fine with using different Cartesian coordinate systems in geometry? What about using spherical coordinates?I know a good book … 😁
I am getting confused even if we going to switch between cartesian and spherical coordinates for the same physical problem.

A book on tensor calculus or on "relativity without tensor calculus"?
 
  • Like
Likes Shreya
  • #59
Delta2 said:
A book on tensor calculus or on "relativity without tensor calculus"?
A good book for learning tensor calculus ... 😉

Although to be fair, most of introductory special relativity is perfectly accessible with just vector analysis.
 
  • Like
Likes Shreya and Delta2
  • #60
Shreya said:
I think he just wants you to re-ask your question in post #49 by replacing ##t## with ##T## wherever applicable. Example, You have - "##t## are maximum" ##\rightarrow## ##T## are maximum.
And In post #53, you said "##u## and ##t##" are fixed, while you should have said ##u## and ##T## are fixed. (Cause any choice of ##u## or ##v## doesn't fix the independent ##t## but it does fix ##T##)
It may not seem like a big difference - but it is. ##t## is the independent continuous variable as @PeroK mentioned while ##T## is the impact time.
Moreover you are minimizing ##u(T)## not ##u(t)## & the graphs given were of ##u(T)##. Also note that ##u## doesn't depend on ##t## but It does on ##T##
It's my fault - because I used the wrong notation first and caused this confusion 😕.
Yes, that's what I meant
 

Similar threads

  • · Replies 20 ·
Replies
20
Views
2K
Replies
25
Views
2K
  • · Replies 6 ·
Replies
6
Views
1K
  • · Replies 1 ·
Replies
1
Views
1K
  • · Replies 7 ·
Replies
7
Views
2K
  • · Replies 21 ·
Replies
21
Views
1K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 5 ·
Replies
5
Views
2K
  • · Replies 2 ·
Replies
2
Views
973
  • · Replies 27 ·
Replies
27
Views
4K