Angled Length Contraction (Relativity)

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Homework Help Overview

The discussion revolves around the calculation of the length of a meter stick that is angled at 60 degrees relative to the direction of motion in the context of special relativity, specifically addressing length contraction effects at a velocity of 0.8c.

Discussion Character

  • Exploratory, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants explore the application of Lorentz transformations and the implications of the angle of the meter stick in different reference frames. Questions arise regarding the definitions of variables and the correct interpretation of angles in the lab frame versus the rest frame of the stick.

Discussion Status

Some participants have provided insights into the relationships between the components of the meter stick's length in different frames. There is an ongoing exploration of how to correctly apply the Lorentz transformations to find the contracted length, with various interpretations being discussed. A participant has arrived at a calculation that aligns with the expected answer, indicating a productive direction in the discussion.

Contextual Notes

Participants note the importance of distinguishing between the lab frame and the rest frame of the meter stick, as well as the implications of using unit lengths in calculations. The discussion also highlights the need for clarity in defining angles and lengths in different reference frames.

Blanchdog
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Homework Statement


Find the length of a meter stick if in the laboratory frame it is angled at 60 degrees relative to the direction of motion, and it is traveling at .8 c.

I have calculated gamma to be 1.667

Homework Equations


Lorentz transformations

The Attempt at a Solution


a' = l' cos(x), b = l' sin(x)
a = cos(60), b = sin(60)
a' = a/gamma, b' = b
l' cos(x) = cos(60)/gamma, l' sin(x) = sin(60)
combine by eliminating l'
cos(60)/(cos(x) gamma) = sin(60)/sin(x)
tan(x) = tan(60) gamma
x = arctan(tan(60) gamma)
plug x back into solve for l'

l' = cos(60)/(cos(x) gamma)

This gives me a result of about 91 cm, but the book says it should be 82 cm. Where did I go wrong?
 
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Blanchdog said:

Homework Statement


Find the length of a meter stick if in the laboratory frame it is angled at 60 degrees relative to the direction of motion, and it is traveling at .8 c.

I have calculated gamma to be 1.667

Homework Equations


Lorentz transformations

The Attempt at a Solution


a' = l' cos(x), b = l' sin(x)
a = cos(60), b = sin(60)
a' = a/gamma, b' = b
l' cos(x) = cos(60)/gamma, l' sin(x) = sin(60)
combine by eliminating l'
cos(60)/(cos(x) gamma) = sin(60)/sin(x)
tan(x) = tan(60) gamma
x = arctan(tan(60) gamma)
plug x back into solve for l'

l' = cos(60)/(cos(x) gamma)

This gives me a result of about 91 cm, but the book says it should be 82 cm. Where did I go wrong?

I can't follow what you are trying to do at all. When you say ##a = \cos(60)##, what is ##a##?
 
PeroK said:
I can't follow what you are trying to do at all. When you say ##a = \cos(60)##, what is ##a##?

I'm treating the meter stick as the hypotenuse of a right triangle. a is aligned with the x-axis (the direction of motion) and b is aligned with the y-axis (perpendicular to the direction of motion).
 
Blanchdog said:
I'm treating the meter stick as the hypotenuse of a right triangle. a is aligned with the x-axis (the direction of motion) and b is aligned with the y-axis (perpendicular to the direction of motion).

In what frame is this? If you are in the rest frame of the stick, then the angle is not ##60°##. And if you are in the lab frame, then the lengths are not simply ##\cos## and ##\sin## as the stick is not of unit length in this frame.
 
`
PeroK said:
In what frame is this? If you are in the rest frame of the stick, then the angle is not ##60°##. And if you are in the lab frame, then the lengths are not simply ##\cos## and ##\sin## as the stick is not of unit length in this frame.

The angle is 60 degrees in the lab frame, meaning that the angle in the frame of the meter stick will be larger than 60 degrees. I denote this by x in the problem. And I can see why the I cannot use a unit length there, but I'm not sure how I can solve it since I know either l and don't know the angle or I know the angle and don't know l, depending on the reference frame. In this case, I need to figure out l (l') in the lab reference frame. I feel like there should be some sort of Lorentz angle transformation, but I've only see that for velocities, not distances.
 
Blanchdog said:
`The angle is 60 degrees in the lab frame, meaning that the angle in the frame of the meter stick will be larger than 60 degrees. I denote this by x in the problem. And I can see why the I cannot use a unit length there, but I'm not sure how I can solve it since I know either l and don't know the angle or I know the angle and don't know l, depending on the reference frame. In this case, I need to figure out l (l') in the lab reference frame. I feel like there should be some sort of Lorentz angle transformation, but I've only see that for velocities, not distances.

What do you know in the lab frame? Write down what you can. Hint: take the length in the lab frame to be ##L## with ##L^2 = a^2 + b^2##, where ##a, b## are the components of length in the direction of motion and perpendicular to the direction of motion respectively.

Hint: forget the angle in the rest frame of the rod - you don't need it.

Suggestion: use ##v, \gamma, \theta## and solve the problem generally. At this level, you should be using algebra - for many reasons - in preference to plugging in numbers at the outset.
 
PeroK said:
What do you know in the lab frame? Write down what you can.

Going to change notation here from above, everything denoted with a subscript 0 like this (X0) will be the value for the meter stick's frame, everything without a subscript will be in the lab reference frame.

Lab Reference Frame:
L2 = a2 + b2
v = .8 c
γ = 1.667
a = a0 / γ
b = b0
a = L cos (θ)
b = L sin (θ)

Meter stick reference frame:
L0 = 1
L02 = a02 + b02

Substituting into the final expression above:

L02 = (aγ)2 + b2
L02 = (L cos(θ) γ)2 + (L sin(θ))2
L02 = L2 ((cos(θ) γ)2 + (sin(θ))2)
L = √(L02/(cos(θ)2 γ2 + sin(θ)2))

Plugging in numbers:

L = √(1/(cos(60)2 * 1.6672 + sin(60)2))
L = .832 m, which is the correct answer! Thanks for the help.
 
Last edited:
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As an aside, you can see the relationship between the angles is:

##\tan(\theta) = \frac{b}{a} = \frac{b_0}{a_0/\gamma} = \gamma \frac{b_0}{a_0} = \gamma \tan(\theta_0)##
 
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