2.3.33 · D4Modern Physics

Exercises — General relativity — equivalence principle, curved spacetime (overview)

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Some constants we reuse throughout — earn them once, use them everywhere:


Level 1 — Recognition

L1.1

Which statement is the Einstein equivalence principle (not the weak one)? (a) All objects fall at the same rate. (b) A freely-falling sealed lab is indistinguishable from a lab floating in deep space. (c) Inertial mass equals gravitational mass.

Recall Solution

(b).

  • (a) and (c) are the weak equivalence principle — they only talk about falling and masses.
  • (b) is the Einstein version: it upgrades the statement to all of physics inside the box, not just falling. That "you can't tell the difference with any experiment" is the extra bite that lets Einstein turn gravity into geometry.

L1.2

A "geodesic" is best described as: (a) the shortest path in flat space only, (b) the straightest possible path through curved spacetime, (c) a circular orbit.

Recall Solution

(b). A geodesic is the generalisation of "straight line" to a curved surface — it is the path you follow when no force pushes you sideways. A free-faller travels a geodesic. See Geodesics & Curvature.


Level 2 — Application

L2.1 — Universal falling

Two balls, masses (a marble) and (a shot-put), are dropped in vacuum. Using , find the acceleration of each.

Recall Solution

WHAT: Newton's 2nd law ; gravity . Set equal. WHY the masses cancel: the equivalence principle says for everything, so regardless of mass. The marble and the shot-put accelerate identically. Mass never enters the answer — that cancellation is the seed of GR.

L2.2 — Pound–Rebka redshift

Light climbs a tower of height in field . Compute the fractional frequency shift .

Recall Solution

WHY this formula: a photon climbing out of a gravity well loses "effective energy," so its frequency drops — this is Gravitational Time Dilation read as a colour shift. Tiny — but Pound and Rebka measured it in 1959.

L2.3 — Light bends in the elevator

A laser crosses a box of width while the box accelerates upward at . How far does the beam appear to "fall"?

Figure — General relativity — equivalence principle, curved spacetime (overview)
Recall Solution

WHAT (look at the figure): the beam travels straight in space, but the box rises under it, so from inside the beam curves down.

  • Time to cross: .
  • Box rises like any accelerating thing: . WHY it matters: By the Einstein EP, the same bend must happen in real gravity — gravity bends light. See Gravitational Lensing.

Level 3 — Analysis

L3.1 — Two clocks on a tower

A clock at the base of a tower and one at the top. Which runs faster, and by what fractional rate ?

Recall Solution

WHICH is faster: the top clock — higher gravitational potential means faster ticking. So the top clock gains about seconds per second — over one full day ( s) that is roughly s ns.

L3.2 — Why the "force" picture breaks

Two balls are released apart, both above Earth's surface, from rest. Explain qualitatively why they approach each other as they fall, and name the phenomenon.

Figure — General relativity — equivalence principle, curved spacetime (overview)
Recall Solution

WHAT (see figure): each ball falls toward Earth's centre, not "straight down parallel." Two lines aimed at the same centre must converge. WHY this kills the force picture: you can cancel gravity in one small box by free-falling — but you cannot make both balls' paths straight at once. This irreducible convergence of free-fallers is the tidal effect, and it is exactly what mathematicians call spacetime curvature. See Geodesics & Curvature.

L3.3 — GPS: which correction dominates?

For a GPS satellite the gravitational (GR) effect makes its clock run faster by about ; the velocity (SR) effect makes it run slower by about . What is the net daily drift, and why must both be included?

Recall Solution

WHAT: the two effects have opposite signs, so add them: WHY both: velocity (SR, Special Relativity) always slows a moving clock; altitude (GR) speeds a high clock. GPS is high and fast, so both matter. Ignore either and positions drift kilometres per day. See GPS Corrections.


Level 4 — Synthesis

L4.1 — Newtonian light-bending is half

The full GR deflection of starlight grazing the Sun is (arcseconds). A naive "photon-with-mass" Newtonian calculation gives exactly half. If your Newtonian estimate came out , what does the factor-of-2 discrepancy tell you physically?

Recall Solution

WHAT: exactly. WHY the factor 2: Newtonian gravity only curves the time part of spacetime (energy in a potential). GR curves both space and time, and the space-curvature contributes an equal second half. The photon "falls" through curved time and rides curved space — two equal contributions. The lesson: matching Newton isn't enough; the extra factor of 2 (measured by Eddington, 1919) is a direct fingerprint of space itself being curved, not just a force acting.

L4.2 — Build the redshift from a climbing photon

Starting only from "a photon has effective mass " and "climbing height costs potential energy per unit mass ," derive . State WHAT and WHY at each step.

Recall Solution

Step 1 — photon's effective mass. Energy (Planck), and mass-energy , so effective mass . WHY: to talk about a photon "climbing" against gravity we need something for gravity to grab — its energy plays the role of mass. Step 2 — energy lost climbing height . Potential energy gained . WHY: lifting mass by height in field costs — standard mechanics. Step 3 — the photon pays with its own energy. It cannot slow down (light is always ), so it pays by losing frequency: Divide by : WHAT it means: the minus sign = the frequency drops climbing up (redshift). The receiver's clock therefore ticks faster by the same .


Level 5 — Mastery

L5.1 — GPS from potential energy, end to end

A GPS satellite orbits at radius from Earth's centre; the ground receiver sits at . Earth's mass . Using the potential form compute the gravitational daily gain (in microseconds over ). Explain each piece.

Recall Solution

WHY this formula: the Newtonian potential is . A clock higher up (less negative ) runs faster; the fractional rate difference is . We want (satellite − ground), and since , the satellite gains. Numbers: Over one day: WHAT it means: this recovers the famous "s/day" gravitational speed-up — the number your phone corrects for every day. See GPS Corrections.

L5.2 — The whole chain, in words

In 4–6 sentences, connect: inertial = gravitational massequivalence principlelight bending & time dilationtidal effects can't be removedcurved spacetime & geodesics.

Recall Solution

The chain: Experiment shows to , so all objects fall identically — mass cancels. Einstein promoted this to the equivalence principle: a free-falling lab is locally indistinguishable from no gravity, and an accelerating box mimics a gravitational field. From the accelerating box we derive that light bends (the floor rises under the beam) and clocks lower down run slow (climbing photons redshift). But the box trick only works locally — two distant free-fallers still converge toward Earth's centre, a tidal effect no free-fall frame can erase. That irreducible convergence is spacetime curvature, so gravity is not a force but geometry: matter curves spacetime (), and free objects glide along geodesics — "matter tells spacetime how to curve; spacetime tells matter how to move."


Wrap-up recall

Recall One-line answers (hide first!)

Einstein EP in one line ::: A freely-falling lab is locally indistinguishable from one with no gravity. Why does mass cancel in free fall ::: Because for everything, so independent of mass. Sign of GPS net drift ::: Positive — satellite clock runs s/day fast. What can't free-fall remove ::: Tidal effects — the convergence of nearby geodesics = curvature. Newtonian light bending vs GR ::: Newton gives exactly half; GR adds the equal space-curvature part.


Connections