Einstein’s proof of E = mc^2

academics math
By Noah M.

In this post, we’re going to prove the most famous formula in all of science, E = mc^2! We’ll do this using a simplified version of Einstein’s original 1905 proof. In this post I will assume that you are familiar with special relativity and Lorentz transformations.

Consider a box of mass m which is at rest. At a certain moment, it spontaneously releases two photons of wavelength λ moving in opposite directions.

Screen Shot 2022-04-26 at 3.14.22 PM

The energy of a photon is given by

Screen Shot 2022-04-26 at 3.14.55 PMand the momentum of a photon is given by

Screen Shot 2022-04-26 at 3.15.31 PMThis means that, in order for energy to be conserved, the box must lose two photons worth of energy:

Screen Shot 2022-04-26 at 3.16.42 PMLet’s now consider this exact same scenario in another reference frame. Namely, let’s consider the reference frame where the box is moving with some velocity v

The wavelengths of the two photons will be different in this reference frame. In fact, one of the photons will be “blueshifted” (its wavelength will shrink) and the other photon will be “redshifted” (its wavelength will expand). Let’s derive a formula for how the wavelength of a photon is changed when we shift reference frames.

To do this, notice that the equation of a wave moving to the right is

Screen Shot 2022-04-26 at 3.17.47 PMA photon is a wave of light, and is more or less described by the above equation. (We will not worry about what is waving, or what is the amplitude of this wave. All we need to know is that a photon is some sort of wave, as above.)

We can use the formula for a Lorentz transformation to express the old coordinates, t and x, in terms of the new coordinates t’ and x’.

Screen Shot 2022-04-26 at 3.18.32 PMLet us now re-express the quantity x - ct, which appears in our equation for the wave, in terms of the new coordinates x’ and t’. In order to do this, we simply plug our above expressions for t and x into the expression x - ct. We then find, after a bit of algebra,

Screen Shot 2022-04-26 at 3.19.24 PM

Plugging this into our expression for a wave, we get

Screen Shot 2022-04-26 at 3.20.01 PMIf we stare at the right hand side of the above equation, we realize that the wavelength λ’ in the new frame is simply equal to

Screen Shot 2022-04-26 at 3.20.37 PMwhich is what we wanted to show.

Now, from here on out, we’re going to make a simplifying approximation. We’re going to assume that our velocity v is much smaller than c. Therefore, we’re going to drop all terms which are second order in v. For instance, when we do this, the Lorentz factor γ is approximately equal to 1. This is because if we do a Taylor expansion, we find that the first non-trivial correction to γ is second order in v and can be ignored:

Screen Shot 2022-04-26 at 3.47.34 PMUsing this first order approximation, we therefore have that the momentum of the right-moving photon is equal to

Screen Shot 2022-04-26 at 3.48.07 PM

For the left moving photon, we have to modify this expression slightly. We have to switch v with -v because the photon is moving in the opposite direction of v, and we have to put an overall minus sign in front of the expression because the photon is moving in the other direction. All in all, the momentum of the left-moving photon is

Screen Shot 2022-04-26 at 3.48.45 PM

A picture of the situation is as follows:

Screen Shot 2022-04-26 at 3.49.20 PM

Therefore, the combined change in momentum due to the emission of the two photons is

Screen Shot 2022-04-26 at 3.49.45 PMFurthermore, because momentum must be conserved, the change in momentum of the box must be equal to

Screen Shot 2022-04-26 at 3.50.25 PM

We are nearing the punch line.

Notice that, before and after the box emits the photons, it must be traveling at the v, meaning its velocity doesn’t change. (This can be seen by remembering we are looking at our stationary box in a moving reference frame.) Recall that the momentum of the box is equal to p = mv. (This formula for the momentum of the box is actually modified for velocities comparable to c, but because we’re only concerned about terms to the first order in v, we don’t have to worry about that and can use the non-relativistic formula.)

Therefore, because the momentum of the box must change after the photons are emitted, and because the velocity must stay the same, we can conclude the mass of the box must change!

Screen Shot 2022-04-26 at 3.50.52 PMThis is a mind boggling result!

Equating the above two expressions, we know the mass must change by exactly

Screen Shot 2022-04-26 at 3.51.26 PMWe are almost done! If we massage this formula a little, we can re-express the change in mass in terms of the change in the rest energy of the box.

Screen Shot 2022-04-26 at 3.52.01 PM


Screen Shot 2022-04-26 at 3.52.26 PM

and we are done!


academics study skills MCAT medical school admissions SAT expository writing college admissions English MD/PhD admissions GRE GMAT LSAT chemistry writing strategy math physics ACT biology language learning test anxiety graduate admissions law school admissions MBA admissions interview prep homework help creative writing AP exams MD study schedules summer activities career advice history personal statements academic advice premed philosophy secondary applications Common Application computer science organic chemistry ESL PSAT economics grammar test prep admissions coaching law statistics & probability supplements psychology SSAT covid-19 legal studies 1L CARS logic games reading comprehension Spanish USMLE calculus dental admissions parents research Latin engineering verbal reasoning DAT excel mathematics political science French Linguistics Tutoring Approaches chinese DO MBA coursework Social Advocacy academic integrity case coaching classics diversity statement genetics geometry kinematics medical school skills IB exams ISEE MD/PhD programs PhD admissions algebra astrophysics athletics biochemistry business business skills careers data science letters of recommendation mental health mentorship quantitative reasoning social sciences software engineering trigonometry work and activities 2L 3L Academic Interest Anki EMT English literature FlexMed Fourier Series Greek Italian MD vs PhD Pythagorean Theorem STEM Sentence Correction Zoom admissions advice algorithms amino acids analysis essay architecture argumentative writing art history artificial intelligence cantonese capacitors capital markets cell biology central limit theorem chemical engineering chromatography climate change clinical experience cold emails community service constitutional law curriculum dental school distance learning enrichment european history finance first generation student fun facts functions gap year harmonics health policy history of medicine history of science information sessions institutional actions integrated reasoning intern international students internships investing investment banking logic mandarin chinese mba meiosis mitosis music music theory neurology operating systems phrase structure rules plagiarism poetry pre-dental presentations proofs pseudocode school selection simple linear regression sociology software study abroad teaching tech industry transfer typology units virtual interviews writing circles