Particle moving at speed ##bc## relative to laboratory frame

In summary, the discussion focuses on a particle traveling at a speed denoted as ##bc## in relation to a laboratory frame. This scenario typically involves relativistic effects, where the behavior of the particle is analyzed using principles of special relativity. Key considerations include the implications of such high velocities on time dilation, length contraction, and energy-momentum relationships, which are essential for understanding the particle's dynamics and interactions within the laboratory environment.
  • #1
member 731016
Homework Statement
Please see below
Relevant Equations
Please see below
For this problem,
1715724165695.png

My working is

(a) ## \Delta t = \frac{a}{\sqrt{1 - b^2}}~ns ##
(b) ## \frac{abc}{(1 \times 10^9)\sqrt{1 - b^2}}~m= d_1 ##
(c) By symmetry, ##d_2 = -d_1##

##-\frac{abc}{(1 \times 10^9) \sqrt{1 - b^2}}~m= d_2##, however, I'm not sure whether my explanation for (c) is enought, does someone please know how to explain it better?

Thanks!
 
Last edited by a moderator:
Physics news on Phys.org
  • #2
It is not enough as it is incorrect. The particle lifetime in its rest frame is not the same as in the lab frame.
 
  • Love
Likes member 731016
  • #3
You don't seem to have used ##a## at all.

For (c), think about what the particle frame says about the lab's velocity. Is it consistent with your answer?
 
  • Love
Likes member 731016
  • #4
Orodruin said:
It is not enough as it is incorrect. The particle lifetime in its rest frame is not the same as in the lab frame.
Ibix said:
You don't seem to have used ##a## at all.

For (c), think about what the particle frame says about the lab's velocity. Is it consistent with your answer?
Thank you for your replies @Orodruin and @Ibix!

Sorry there was a typo in my working, what I was intending was this:

(a) ## \Delta t = \frac{a}{\sqrt{1 - b^2}}~ns ##
(b) ## \frac{abc}{(1 \times 10^9)\sqrt{1 - b^2}}~m= d_1 ##
(c) By symmetry, ##d_2 = -d_1##

##-\frac{abc}{(1 \times 10^9) \sqrt{1 - b^2}}~m= d_2##

Thanks!
 
  • #5
ChiralSuperfields said:
(c) By symmetry, ##d_2 = -d_1##
This argument is still wrong.
 
  • Love
Likes member 731016
  • #6
Orodruin said:
This argument is still wrong.
Thank you for your reply @Orodruin!

Do you please know why? Going from the spaceship frame and the earth frame should be symmetrical should it not?

Thanks!
 
  • #7
Using the number ##(1 \times 10^9)## in (b) and (c) is also wrong.
 
  • Love
Likes member 731016
  • #8
Hill said:
Using the number ##(1 \times 10^9)## in (b) and (c) is also wrong.
Thank you for your reply @Hill!

Do you please know why it is wrong? The ##(1 \times 10^9)## factor comes from converting the time in nanoseconds to the time in seconds

Thanks!
 
  • #9
ChiralSuperfields said:
Thank you for your reply @Hill!

Do you please know why it is wrong? The ##(1 \times 10^9)## factor comes from converting the time in nanoseconds to the time in seconds

Thanks!
Why do you convert?
 
  • Love
Likes member 731016
  • #10
Hill said:
Why do you convert?
Thank you for your reply @Hill!

So that I can I get the distance in ##m##.

Thanks!
 
  • #11
ChiralSuperfields said:
Thank you for your reply @Hill!

So that I can I get the distance in ##m##.

Thanks!
1. There is no such requirement in the problem.
2. It does not ensure that you will get the distance in ##m##, anyway.
 
  • Love
Likes member 731016
  • #12
Thank you for your reply @Hill! So removing the factor ##1 \times 10^9## gives the correct solution thought?


(a) ## \Delta t = \frac{a}{\sqrt{1 - b^2}} ##
(b) ## \frac{abc}{\sqrt{1 - b^2}} = d_1 ##
(c) By symmetry, ##d_2 = -d_1##

##-\frac{abc}{\sqrt{1 - b^2}} = d_2##

Thanks!
 
  • #13
ChiralSuperfields said:
Thank you for your reply @Hill! So removing the factor ##1 \times 10^9## gives the correct solution thought?


(a) ## \Delta t = \frac{a}{\sqrt{1 - b^2}} ##
(b) ## \frac{abc}{\sqrt{1 - b^2}} = d_1 ##
(c) By symmetry, ##d_2 = -d_1##

##-\frac{abc}{\sqrt{1 - b^2}} = d_2##

Thanks!
The answer to (c) is still wrong, as is said in #5.

If it were correct, then the laboratory has moved in the particle's reference frame during the lifetime of the particle the distance ##\frac{abc}{\sqrt{1 - b^2}}##. It moved with the speed ##bc##. Thus, the lifetime of the particle in the particle's reference frame was ##\frac{abc}{(\sqrt{1 - b^2})(bc)} = \frac{a}{\sqrt{1 - b^2}}##. But it should be ##a##. You get a contradiction.
 
  • Love
Likes member 731016
  • #14
Hill said:
The answer to (c) is still wrong, as is said in #5.

If it were correct, then the laboratory has moved in the particle's reference frame during the lifetime of the particle the distance ##\frac{abc}{\sqrt{1 - b^2}}##. It moved with the speed ##bc##. Thus, the lifetime of the particle in the particle's reference frame was ##\frac{abc}{(\sqrt{1 - b^2})(bc)} = \frac{a}{\sqrt{1 - b^2}}##. But it should be ##a##. You get a contradiction.
Thank you for your reply @Hill!

Sorry do you please know how to what the asymmetry is between the results? I don't understand how to find the asymmetry between them.

Thanks!
 
  • #15
ChiralSuperfields said:
Thank you for your reply @Hill!

Sorry do you please know how to what the asymmetry is between the results? I don't understand how to find the asymmetry between them.

Thanks!
There is asymmetry in the distances like there is asymmetry in the lifetimes.
 
  • Love
Likes member 731016
  • #16
ChiralSuperfields said:
Sorry do you please know how to what the asymmetry is between the results? I don't understand how to find the asymmetry between them.
See #3. What is the lab's velocity in the particle frame?
 
  • Love
Likes member 731016
  • #17
Ibix said:
See #3. What is the lab's velocity in the particle frame?
In particle frame, particle is at rest, lab is moving. In lab frame, lab is at rest, particle is moving.

In particle frame, particle is at rest, lab is moving at ##-bc## (##bc## to the left).

In lab frame, lab is at rest, particle is moving at ##bc## to the right.

Is that please what you were getting at?

Thanks!
 
  • #18
ChiralSuperfields said:
In particle frame, particle is at rest, lab is moving at ##-bc## (##bc## to the left).
Yes. So how far does the lab move according to the particke frame?
 
  • Love
Likes member 731016
  • #19
Ibix said:
Yes. So how far does the lab move according to the particke frame?
Thank you for yor reply @Ibix! I'll think about it overnight and get back to you in tomorrow!
 
  • #20
Ibix said:
Yes. So how far does the lab move according to the particke frame?
THank you for your reply @Ibix! ##v\Delta t = d##

##-bca = d##.

Is that please correct?

Thanks!
 
  • #21
ChiralSuperfields said:
THank you for your reply @Ibix! ##v\Delta t = d##

##-bca = d##.

Is that please correct?

Thanks!
Looks right to me.
 
  • Love
Likes member 731016

FAQ: Particle moving at speed ##bc## relative to laboratory frame

1. What does it mean for a particle to move at speed ##bc##?

In physics, the term "speed ##bc##" refers to a particle moving at a speed that is a fraction of the speed of light, denoted by ##c##. The ##b## is typically a dimensionless parameter representing the ratio of the particle's speed to the speed of light, where ##b = v/c##. If a particle is said to move at speed ##bc##, it means its velocity is ##v = b \cdot c##.

2. How does relativistic physics apply to a particle moving at speed ##bc##?

When a particle moves at a significant fraction of the speed of light (i.e., when ##b## is close to 1), relativistic effects become significant. According to Einstein's theory of relativity, as the speed of a particle approaches the speed of light, its relativistic mass increases, time dilation occurs, and lengths contract in the direction of motion. This means that measurements of time and distance are not the same in the laboratory frame compared to the particle's rest frame.

3. What happens to the particle's mass as it approaches speed ##bc##?

As a particle accelerates towards the speed of light, its relativistic mass increases according to the equation ##m = \frac{m_0}{\sqrt{1 - b^2}}##, where ##m_0## is the rest mass of the particle. This means that it requires increasingly more energy to continue accelerating the particle as it gets closer to the speed of light, effectively making it impossible for any particle with mass to reach or exceed the speed of light.

4. How is energy related to a particle moving at speed ##bc##?

The total energy of a particle moving at speed ##bc## can be described by the relativistic energy equation: ##E = \gamma m_0 c^2##, where ##\gamma = \frac{1}{\sqrt{1 - b^2}}## is the Lorentz factor. As the particle's speed increases and approaches the speed of light, the Lorentz factor increases, leading to a significant increase in the total energy of the particle, which includes both its rest mass energy and its kinetic energy.

5. How does the laboratory frame perceive the time experienced by the particle moving at speed ##bc##?

In the laboratory frame, time for the particle moving at speed ##bc## is experienced differently due to time dilation. According to the time dilation formula, the time experienced by the moving particle (proper time) is related to the time measured in the laboratory frame by the equation: ##\Delta t' = \Delta t \cdot \sqrt{

Back
Top