C’è tempo? Come lo sappiamo?

Come facciamo a sapere che il tempo esiste?

Tutta la nostra vita è regolata dagli orologi, ma ciò che misurano è meno certo. Come possiamo essere sicuri che il tempo esista davvero? È ora di parlare con l’esperta Kazuya Koyama.

La sveglia suona al mattino. Prendi il tuo treno mattutino per l’ufficio. Fai una pausa pranzo. Prendi il treno della sera per tornare. Vai per un’ora. cenando. vai a letto. si ripete. Si celebrano i compleanni, si registrano gli anniversari e si commemorano i decessi. Nascono nuove nazioni, sorgono e cadono imperi.

Tutta l’esistenza umana è legata al passare del tempo. Tuttavia, non possiamo vederlo né possiamo toccarlo. Quindi, come facciamo a sapere che esiste davvero?

“In fisica, abbiamo quella che chiamiamo l’idea di ‘tempo assoluto’ ed è usata per descrivere vari cambiamenti come una serie di eventi”, ha esordito Koyama. “Usiamo la fisica newtoniana per descrivere come si muovono le cose e il tempo ne è una componente essenziale”. Koyama è Professore di Cosmologia presso l’Istituto di Cosmologia e Gravitazione a[{” attribute=””>University of Portsmouth.

To this day, classic Newtonian thought on time – where time is constant throughout the universe – is still a good approximation of how humans experience time in their daily lives. We all experience time in the same way and we all synchronize our clocks in the same way, no matter where we are in the world, whether that be London, Tokyo, New York, or Buenos Aires.

There’s no time without space

Physicists though have discovered that time can actually behave differently and is not as consistent as Newton thought.

“When we speak of time, we need to think of space as well – they come in a package together,” Koyama says. “We cannot disconnect the two, and the way that an object moves through space determines how it experiences time.”

In short, the time you experience depends on your velocity through space as the observer. This works as outlined through Einstein’s special relativity, a theory of how speed impacts mass, time, and space. Additionally, according to Einstein’s general theory of relativity, the gravity of a massive object can impact how quickly time passes. Many experiments have been undertaken that have since proven this to be true.

Physicists have even found that black holes warp the immediate space-time around them due to their immense gravitational fields. Supported by the European Research Council, Koyama continues to investigate this theory.

“A good, solid example to get your head around all of this is to look at how we use GPS,” Koyama continues. “GPS works due to a network of satellites orbiting the Earth. They’re placed at a very high altitude and thus the gravity they experience is weaker. Therefore, time should actually go faster for them than it does for us on the ground, where we experience higher gravity. But because the satellites are traveling at very high speeds around the planet, this in effect helps to slow time down, compensating for the lack of gravity.”

Understanding how these two effects work and influence each other is essential for ensuring that the global GPS network functions correctly. And a crucial ingredient in this is a consistent theory of time that explains how objects move. So clocks aren’t telling us falsehoods: time indeed exists outside of our own perception.

Could we ever go backward in time?

Finally, the question of whether time travel could one day be possible had to be put before Koyama. As a professor of cosmology at the University of Portsmouth, he is best placed to tell us the truth.

“I’m sorry to disappoint you but for time travel to be possible, we would need to discover a completely new type of matter that has the power to change the curvature of time and space,” Koyama says. “Such matter would require properties that simply do not exist in nature. We physicists strongly believe that going back to the past is simply impossible – but it’s nice to fantasize about it.”

Click here to find out more about Koyama’s research: Challenging the general theory of relativity

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