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Tachyonic antitelephone

Tachyonic antitelephone is a physics topic covered in the lgStudy science library. This page brings together a partial reference excerpt, illustrations, worked examples, real-world applications and a short study plan, so you can understand Tachyonic antitelephone rather than just read about it. In short: A tachyonic antitelephone is a hypothetical device in theoretical physics that could be used to send signals into one's own past. Albert Einstein in 1907 presented a thought experiment of how faster-than-light signals can lead to a paradox of causality, which was described by Einstein and Arnold Sommerfeld in 1910 as a means "to telegraph into the past".

Tachyonic antitelephone — main illustration
Tachyonic antitelephone — illustration

Key takeaways

  • Tachyonic antitelephone belongs to physics; place it in that map before memorising details.
  • Learn the definition first, then one example that makes the definition concrete.
  • Connect Tachyonic antitelephone to a quantity you can measure, compute or draw — that is where exam questions come from.
  • Reproduce the core statement of Tachyonic antitelephone from memory before moving on to harder problems.

Reference excerpt

A tachyonic antitelephone is a hypothetical device in theoretical physics that could be used to send signals into one's own past. Albert Einstein in 1907 presented a thought experiment of how faster-than-light signals can lead to a paradox of causality, which was described by Einstein and Arnold Sommerfeld in 1910 as a means "to telegraph into the past". The same thought experiment was described by Richard Chace Tolman in 1917; thus, it is also known as Tolman's paradox. A device capable of "telegraphing into the past" was later also called a "tachyonic antitelephone" by Gregory Benford, David Book, and William Newcomb. According to the current understanding of physics, no such faster-than-light transfer of information is possible.

One-way example

Tolman used the following variation of Einstein's thought experiment: Imagine a distance with endpoints A {\displaystyle A} and B {\displaystyle B} . Let a signal be sent from A propagating with velocity a {\displaystyle a} towards B. All of this is measured in an inertial frame where the endpoints are at rest. The arrival at B is given by:

Δ t = t 1 − t 0 = B − A a . {\displaystyle \Delta t=t_{1}-t_{0}={\frac {B-A}{a}}.}

Here, the event at A is the cause of the event at B. However, in the inertial frame moving with relative velocity v, the time of arrival at B is given according to the Lorentz transformation (c is the speed of light):

Δ t ′ = t 1 ′ − t 0 ′ = t 1 − v B / c 2 1 − v 2 / c 2 − t 0 − v A / c 2 1 − v 2 / c 2 = 1 − a v / c 2 1 − v 2 / c 2 Δ t . {\displaystyle {\begin{aligned}\Delta t'&=t'_{1}-t'_{0}={\frac {t_{1}-vB/c^{2}}{\sqrt {1-v^{2}/c^{2}}}}-{\frac {t_{0}-vA/c^{2}}{\sqrt {1-v^{2}/c^{2}}}}\\&={\frac {1-av/c^{2}}{\sqrt {1-v^{2}/c^{2}}}}\Delta t.\end{aligned}}}

It can be easily shown that if a > c, then certain values of v can make Δt' negative. In other words, the effect arises before the cause in this frame. Einstein (and similarly Tolman) concluded that this result contains in their view no logical contradiction; he said, however, it contradicts the totality of our experience so that the impossibility of a > c seems to be sufficiently proven.

… excerpt ends here. Continue reading the full article.

Worked examples

Example 1 — a first encounter with Tachyonic antitelephone

Start with the simplest possible case. Write down what Tachyonic antitelephone claims or describes in one sentence, then invent the smallest concrete situation in which that sentence is true. In physics, the smallest case is usually a single object, a single equation or a single measurement. Check that every symbol or term in your sentence has a meaning in that case.

Example 2 — changing one variable

Take the situation from Example 1 and change exactly one quantity: double it, halve it, or set it to zero. Predict what should happen to Tachyonic antitelephone before you calculate. Comparing your prediction with the result is the fastest way to find out whether you understand the idea or only the words.

Example 3 — an exam-style question

Typical questions about Tachyonic antitelephone ask you to (a) state it precisely, (b) apply it to given data, and (c) explain a limitation. Practise writing all three answers in under five minutes; the third part is what separates a full-mark answer from an average one.

Applications of Tachyonic antitelephone

In research
Tachyonic antitelephone appears in physics research whenever the underlying quantities have to be modelled precisely. Papers usually cite it as a starting assumption and then explore where it breaks down.
In technology and industry
Engineering practice reuses Tachyonic antitelephone in design rules, simulations and safety margins. Knowing the idea lets you read a specification sheet and understand why the numbers look the way they do.
In the classroom
Tachyonic antitelephone is common in secondary-school and first-year university syllabi. It links to neighbouring topics Faster-than-light communication, Special relativity, Tachyons, so understanding it makes those chapters shorter.
In everyday life
Look for Tachyonic antitelephone outside the textbook — in sport, cooking, traffic, electronics or the sky above you. An example you found yourself is remembered far longer than one you were given.
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How to study Tachyonic antitelephone in 20 minutes

  1. Read the reference excerpt below once, without taking notes.
  2. Close the page and write down what Tachyonic antitelephone means in your own words.
  3. Compare your version with the excerpt and mark what you missed.
  4. Work through the three examples above with pen and paper.
  5. Explain Tachyonic antitelephone out loud to somebody else — or to Teacher Smith in the lgStudy chat.

Frequently asked questions

What is Tachyonic antitelephone in simple terms?

A tachyonic antitelephone is a hypothetical device in theoretical physics that could be used to send signals into one's own past. Albert Einstein in 1907 presented a thought experiment of how faster-than-light signals can lead to a paradox of causality, which was described by Einstein and Arnold So…

Why does Tachyonic antitelephone matter?

Because it connects several physics ideas at once: it gives you a definition you can apply, a quantity you can calculate, and a way to check whether a result is plausible.

How should I study Tachyonic antitelephone?

Read the excerpt, restate it from memory, then work through the examples and applications listed on this page. The five-step study plan above takes about twenty minutes.

What does this page cover?

It gives you a compact reference excerpt plus original lgStudy explanations, examples, applications and study material on Tachyonic antitelephone.

Tags

  • Faster-than-light communication
  • Special relativity
  • Tachyons
  • Temporal paradoxes
  • Thought experiments in physics

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