The inverse square law is one of the most tested physics concepts on the ARRT exam — and one of the most useful safety tools you'll ever use as a rad tech. In plain terms: double the distance from an X-ray source and the beam intensity drops to a quarter. That single fact shapes how you choose source-to-image distance (SID), how you adjust your exposure factors, and how you protect yourself, your coworkers, and the public every day in the imaging department.
This guide covers the formula, what it means for your technique, worked examples you can actually use, and the exam angles that show up again and again on registry questions.
The inverse square law states that the intensity of radiation is inversely proportional to the square of the distance from the source. In an equation:
I₁ / I₂ = D₂² / D₁²
where I is beam intensity and D is distance from the source.
Why does this happen? Think of the X-ray beam spreading out from a nearly point source into three-dimensional space. As you move farther away, that energy spreads over a larger area — the surface area of a sphere grows with the square of the radius (4πr²). So the same amount of energy is diluted across a bigger surface, and each unit of area receives less X-ray intensity.
The practical punchline:
Distance is the cheapest radiation-protection tool you have. Moving twice as far away doesn't halve your dose — it quarters it. That's the reason every portable radiographer stands far back when exposing, and why control booths and lead barriers make distance so effective.
Formulated for the two situations a technologist actually runs into:
To find intensity (I₂) at a new distance (D₂):
I₂ = I₁ × D₁² / D₂²
To find the safe distance (D₂) needed for a target intensity (I₂):
D₂ = √(I₁ × D₁² / I₂)
Intensity is measured in units like R/hr, mR/hr, or mGy/hr. Distance can be in metres or feet — just keep the units consistent on both sides of the equation.
Example — safe distance: If you measure 100 mR/hr at 1 metre from a source and you want to stand where the intensity is down to 2 mR/hr:
D₂ = √(100 × 1² / 2) = √50 ≈ 7.1 metres
That's why departments hard-wire safety markers, and why technologists keep shielded control areas at a safe distance from the unit rather than right next to it.
You don't just use the inverse square law for safety — you use it for image quality and consistent exposure every time you position a patient. The distance from the focal spot to the image receptor is the source-to-image distance (SID).
| Projection | Typical SID |
|---|---|
| General radiography (most exams) | 40 in (≈100 cm) |
| Erect PA chest / upright chest | 72 in (≈183 cm) |
| Portable/bedside supine chest | 40 in |
Clark's Pocket Handbook for Radiographers specifies the SID for each projection. When you have to change that SID — for a taller patient, a mobile unit, or a decubitus chest — the inverse square law tells you exactly how the exposure must change to keep receptor exposure (and therefore image density) constant. Move the tube farther away and you must increase mAs; move it closer and you must decrease mAs.
Moving from a 40-inch to a 72-inch chest technique isn't a small tweak — it multiplies your mAs by more than 3. Technologists who forget this produce underexposed images and end up repeating the exam, which doubles patient dose. Knowing the direct square law prevents that.
To keep receptor exposure constant when the SID changes, apply the direct square law (also called the density maintenance formula):
mAs₂ = mAs₁ × (D₂ / D₁)²
In words: mAs changes in direct proportion to the square of the distance ratio. This is simply the inverse square law rearranged for technique factors — the exposure you need scales up or down with distance squared.
Example: A portable AP chest is made at 40 in with 4 mAs. You repeat it as an upright chest at 72 in. What mAs keeps the density the same?
mAs₂ = 4 × (72 / 40)² = 4 × 3.24 = 12.96 ≈ 13 mAs
That's a big jump — and exactly why chest technique charts list separate factors for portable (40 in) versus upright (72 in) studies.
| Scenario | Calculation | Result |
|---|---|---|
| Intensity when distance doubles (40→80 in) | 1 / 2² | ¼ (25%) |
| Intensity when distance triples | 1 / 3² | 1/9 (≈11%) |
| 4 mAs at 40 in → change to 60 in | 4 × (60/40)² | 9 mAs |
| 4 mAs at 40 in → change to 72 in | 4 × (72/40)² | ≈13 mAs |
| 4 mAs at 72 in → change to 40 in | 4 × (40/72)² | ≈1.2 mAs |
| Personnel dose 10 mGy/hr at 1 m → at 2 m | 10 / 2² | 2.5 mGy/hr |
| Personnel dose 10 mGy/hr at 1 m → at 4 m | 10 / 4² | 0.625 mGy/hr |
When a registry question doubles the distance, the answer is always ¼ the original intensity. When it asks for a new mAs, plug the distances into mAs₂ = mAs₁ × (D₂/D₁)² and square the distance ratio before multiplying.
The inverse square law is the scientific backbone of the time, distance, and shielding triad taught in every radiation-safety program:
For occupational exposure, this is why you step behind the control shield or stand well clear of the tube during exposure. For public exposure, it's why waiting areas place patients and family members metres away from the primary beam rather than beside the table.
Because the law scales with distance squared, even a modest step back — from 1 m to 2 m — drops your dose fourfold. Two steps back to 4 m drops it sixteenfold. In a busy trauma room where you're exposing repeatedly, that habit meaningfully lowers your cumulative dose over a career. For the full dose picture, see our guide to Radiation Dose Units Explained.
ARRT content specifications establish broad tested categories such as radiation physics and radiation protection. They do not publish a guaranteed number of questions for a narrow topic like the inverse square law — treat it as a high-yield concept, not a fixed question count.
Points that appear again and again:
Practice two worked problems a day until the formula feels automatic. Drawing the flux-spread diagram yourself (source S, circles at 1r, 2r, 3r) is the fastest way to make the "square" drop intuitive.
The inverse square law states that X-ray beam intensity is inversely proportional to the square of the distance from the source. Double the distance and intensity drops to one quarter; triple it and intensity drops to one ninth.
The inverse square law for intensity is I₁/I₂ = D₂²/D₁². For technique work, the direct square law is mAs₂ = mAs₁ × (D₂/D₁)², which keeps receptor exposure constant when the SID changes.
Because beam intensity falls off with the square of distance, you must compensate with mAs (direct square law) so the receptor exposure — and therefore image density — stays constant. Increasing SID requires more mAs; decreasing it requires less.
Use it to place yourself, staff, and the public at a safe distance from the source. Because doubling distance quarters the dose, distance is the most effective low-cost protection measure alongside shielding in the time–distance–shielding triad.
Yes, as a close approximation. At routine clinical SIDs a diagnostic X-ray tube behaves like a point source, so the law is used for both dose calculations and mAs technique adjustments.
The inverse square law governs beam intensity falling off with distance, while image magnification is governed by object-to-image distance and SID geometry. They both involve distance but answer different questions about the image.
Dive deeper into the physics that runs alongside this concept:
Try these ARRT-style multiple choice questions based on this article. Click an option to check your answer — correct answers turn green, wrong ones turn red.