The energy-mass relation E=mc2E = mc^2 is everywhere in physics.

A Gaussian integral:

βˆ«βˆ’βˆžβˆžeβˆ’x2 dx=Ο€ \int_{-\infty}^{\infty} e^{-x^2}\,dx = \sqrt{\pi}

It's on the tip of my tongue. β€” when you almost remember something.

You nailed it. β€” you did it perfectly.

Let's play it by ear. β€” decide as we go.

That rings a bell. β€” sounds familiar.

I'm on the fence. β€” can't decide.

It's a long shot. β€” unlikely to succeed.

Cut to the chase. β€” get to the point.

We're on the same page. β€” we agree.

It slipped my mind. β€” I forgot.