Limit of this expression for apparent length

Click For Summary
SUMMARY

The apparent length of a rod, represented by the expression $$\tilde{L}(x_0) = \gamma L + \beta \gamma \sqrt{D^2 + (\gamma x_0 - \frac{L}{2})^2} - \beta \gamma \sqrt{D^2 + (\gamma x_0 + \frac{L}{2})^2}$$, approaches different limits as $$x_0$$ tends to negative and positive infinity. Specifically, $$\tilde{L}(x_0 \rightarrow -\infty) = \gamma L(1+\beta)$$ and $$\tilde{L}(x_0 \rightarrow \infty) = \gamma L(1-\beta)$$, correcting the initial assumption that both limits equate to $$\gamma L(1-\beta)$$. The key to understanding this discrepancy lies in the careful handling of absolute values in the rearranged expression.

PREREQUISITES
  • Understanding of relativistic length contraction, specifically the Lorentz factor $$\gamma$$.
  • Familiarity with algebraic manipulation of expressions involving square roots.
  • Knowledge of limits in calculus, particularly evaluating expressions as variables approach infinity.
  • Proficiency in handling absolute values in mathematical expressions.
NEXT STEPS
  • Study the properties of the Lorentz factor $$\gamma$$ in special relativity.
  • Learn about the implications of length contraction in relativistic physics.
  • Explore advanced algebra techniques for manipulating expressions with square roots and absolute values.
  • Research limit evaluation techniques in calculus, focusing on expressions involving infinity.
USEFUL FOR

Students and professionals in physics, particularly those focusing on special relativity, as well as mathematicians dealing with limits and algebraic expressions.

etotheipi
Homework Statement
See below
Relevant Equations
N/A
The apparent length of a rod is determined to be$$\tilde{L}(x_0) = \gamma L + \beta \gamma \sqrt{D^2 + (\gamma x_0 - \frac{L}{2})^2} - \beta \gamma \sqrt{D^2 + (\gamma x_0 + \frac{L}{2})^2}$$I am trying to determine expressions for ##\tilde{L}(x_0)## when ##x_0 \rightarrow -\infty## and ##x_0 \rightarrow \infty##. I rearranged it to$$\tilde{L} = \gamma L + \beta \gamma (\gamma x_0 - \frac{L}{2})\sqrt{1+\frac{D^2}{(\gamma x_0 -\frac{L}{2})^2}} - \beta \gamma (\gamma x_0 + \frac{L}{2})\sqrt{1+\frac{D^2}{(\gamma x_0 +\frac{L}{2})^2}}$$And it would then seem in both cases, since the square roots both approach 1 in both limits, that$$\tilde{L}(x_0 \rightarrow -\infty) = \tilde{L}(x_0 \rightarrow \infty)= \gamma L(1-\beta)$$However it is noted in the solution manual that in fact $$\tilde{L}(x_0 \rightarrow -\infty) =\gamma L(1+\beta)$$ and $$\tilde{L}(x_0 \rightarrow \infty) =\gamma L(1-\beta)$$What have I missed? Thanks!
 
Physics news on Phys.org
Careful with signs: ##\sqrt{1+a^2}=|a|\sqrt{(1/a^2)+1}.##
 
  • Like
Likes   Reactions: etotheipi
Infrared said:
Careful with signs: ##\sqrt{1+a^2}=|a|\sqrt{(1/a^2)+1}.##

Ah, yes that's a little subtle... now I'm going to be quite paranoid about this in the future :wink:. It should then be $$\tilde{L} \approx \gamma L + \beta \gamma \left( \left|\gamma x_0 - \frac{L}{2} \right| - \left|\gamma x_0 + \frac{L}{2} \right| \right)$$and that does give the correct result when evaluated. Thanks!
 
Last edited by a moderator:
  • Like
Likes   Reactions: Infrared

Similar threads

  • · Replies 1 ·
Replies
1
Views
3K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 13 ·
Replies
13
Views
4K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 9 ·
Replies
9
Views
2K
  • · Replies 22 ·
Replies
22
Views
4K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 5 ·
Replies
5
Views
1K
Replies
1
Views
1K
  • · Replies 1 ·
Replies
1
Views
2K