Light travels in straight lines: shadows
In a total solar eclipse the dark centre of the Moon’s shadow often covers a strip less than 50 miles wide, while the partial shadow spans a thousand miles or more.
Rays: a simple model of light
Sunlight through a gap in the curtains makes a beam with straight edges, and a torch beam in fog is a straight cone. In a material of the same kind all the way through, light goes in straight lines. Optics uses this to draw light as rays: straight lines with arrows showing which way the light moves. OpenStax calls this part of the subject geometric optics. The ray picture works well as long as the objects the light meets are much larger than its wavelength, which for visible light is less than a micrometre. Mirrors, lenses, cameras and shadows all fall into that range.
We see a lamp because rays from it enter our eyes. We see a book because rays from the lamp hit the book and bounce off in all directions, and some of those rays reach us. Our eyes and brain then assume the light came in a straight line, and place the object back along that line. Most of the time this assumption is right. When it is wrong, for instance when light bends at the surface of water, we see things in places where they are not, which is the subject of a later lesson.
Pinholes and upside-down pictures
A box with a tiny hole in one side and a screen on the other makes a picture without any lens. A ray from the top of a tree can only reach the screen by passing through the hole, so it lands near the bottom of the screen; a ray from the bottom of the tree lands near the top. The picture is upside down. Its size follows from similar triangles: image height ÷ object height = box depth ÷ object distance. A 10 m tree 20 m away seen in a box 10 cm deep makes an image 10 × 0.1 ÷ 20 = 0.05 m, or 5 cm, tall. Darkened rooms with a small hole, called camera obscura, were used by scientists such as Kamal al-Din al-Farisi in his studies of light in the early 1300s, as OpenStax describes.
Sharp shadows and soft shadows
A shadow is the region behind an opaque object that light cannot reach in a straight line. With a very small light source, a point source, every place is either fully lit or fully dark, and the shadow has a sharp edge. Its size again follows from similar triangles. A 4 cm ball 20 cm from a point lamp casts a shadow 4 × 50 ÷ 20 = 10 cm across on a screen 50 cm from the lamp. Move the ball toward the lamp and the shadow grows; move it toward the screen and the shadow shrinks toward the size of the ball.
Most real lights are not points. With a lamp of some size, some places on the screen are hidden from the whole lamp and others from only part of it. The fully dark centre is the umbra, and around it is a lighter ring, the penumbra, where part of the lamp can still be seen. Straight lines from the edges of the lamp past the edges of the object mark the boundaries. The bigger the lamp and the farther the screen, the wider the penumbra and the smaller the umbra; if the lamp is large enough, the umbra disappears entirely and the shadow is soft all over.
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Eclipses: shadows in space
The Sun is a large source, so the Moon and the Earth cast shadows with both an umbra and a penumbra. NASA explains that in a solar eclipse, observers inside the small umbra see the Sun completely blocked, a total eclipse, while those in the much larger penumbra see only part of the Sun covered. As the shadow extends away from the Moon, the umbra narrows, so by the time it reaches the Earth it covers a small area: NASA gives a typical umbral path as less than 50 miles wide, against a penumbra a thousand miles or more across. In a lunar eclipse the Moon passes into the Earth’s shadow instead. Some sunlight bent through the Earth’s atmosphere still reaches it, mostly red, which gives the eclipsed Moon its reddish colour.
- A point lamp, a 4 cm ball 20 cm from the lamp, and a screen 50 cm from the lamp. How wide is the shadow?
- With a point lamp, you move the ball closer to the screen. The shadow…
- Gets smaller
- Gets larger
- Stays the same
- Turns into a penumbra only
- Why does a large lamp give a shadow with a soft edge?
- Some places are hidden from only part of the lamp
- Light curves around large lamps
- Large lamps are brighter
- The ball becomes transparent
- During a solar eclipse you are inside the Moon’s umbra. What do you see?
- A total eclipse
- A partial eclipse
- No eclipse
- A lunar eclipse
- The image in a pinhole camera is…
- Upside down
- Upright and larger
- Always the same size as the object
- Only visible in colour
- A 10 m tree stands 20 m from a pinhole box 0.10 m deep. How tall is the image, in cm?
- Why can you see a sheet of paper that does not give off light itself?
- Light from a lamp bounces off it into your eyes
- Your eyes send out rays that hit it
- Paper stores light
- Paper is a point source
- Lamp 3 cm tall, 4 cm ball 20 cm away, screen at 50 cm. Using umbra = h × D/x − s × (D/x − 1), how wide is the umbra? One decimal place.
- As the Moon’s shadow stretches toward the Earth, its umbra…
- Narrows
- Widens
- Stays the same width
- Turns into a penumbra and then widens
- In one uniform material, light travels in straight lines (rays).
- Pinhole images are upside down; size by similar triangles.
- Point source: sharp shadow. Extended source: umbra plus penumbra.
- Total eclipse inside the umbra, partial eclipse in the penumbra.
Sources for this course (16)
- OpenStax College Physics 2e (openstax.org/books/college-physics-2e): 25.2 The Law of Reflection (θr = θi, diffuse vs mirror reflection, image as far behind the mirror)
- 25.3 The Law of Refraction (Roemer 1676 data -> 2.26 × 10⁸ m/s, about 25% low; Michelson rotating mirrors with a fixed mirror 35 km away, 0.04%; c = 2.99792458 × 10⁸ m/s; n = c/v; Table 25.1 air 1.000293, water 1.333, ice 1.309, crown glass 1.52, flint 1.66, polystyrene 1.49, zircon 1.923, diamond 2.419; Snell's law; 30.0° -> 22.0° gives 1.33; air to diamond 30.0° -> 11.9°; zircon 1.56 × 10⁸ m/s; Ibn Sahl 984; Snell 1580 to 1626; lawn-mower analogy)
- 25.4 Total Internal Reflection (mirror more than 90%; θc = sin⁻¹(n2/n1); polystyrene 42.2°, water 48.6°, diamond 24.4°; fibre optics, cladding; corner reflectors on bicycles and on the Moon; binoculars)
- 25.5 Dispersion (Kamal al-Din al-Farisi 1267 to 1319, camera obscura and a water-filled glass vessel; Theodoric of Freiberg; Ibn al-Haytham; about six rainbow colours; Table 25.2 n at 660/610/580/550/470/410 nm; violet bent most; rainbow seen looking away from the Sun; secondary rainbow from two reflections; lasers disperse little)
- 25.6 Image Formation by Lenses (ray tracing rules, P = 1/f in diopters, 1/do + 1/di = 1/f, m = −di/do, 0.750 m object and f = 0.500 m -> 1.50 m and m = −2.00, magnifier do 7.50 cm -> di −30.0 cm and m = 4.00, Table 25.3 three cases)
- 26.1 Physics of the Eye (cornea and lens act as one thin lens, most bending at the cornea, cornea n 1.38, lens-to-retina 2.00 cm, near point 25 cm, power 50.0 D to 54.0 D, hair 1.20 × 10⁻² cm at 60.0 cm)
- 27.3 (Young 1801)
- NASA science.nasa.gov/eclipses/geometry (umbra, penumbra; typical umbral path may be less than 50 miles wide, penumbra a thousand miles or more) and nasa.gov image article Diagram of Umbra and Penumbra (umbra shrinks, penumbra grows away from the Sun)
- NASA Visible Light page (Newton 1665 prism experiment, 380 to 700 nm)
- Royal Society, Fara 2015 commentary on Newton (1672) New Theory about Light and Colours (royalsocietypublishing.org/rsta/article/373/2039/20140213)
- NIST Meter page (Evenson group 299 792 456.2 ± 1.1 m/s; 1983 definition fixes c = 299 792 458 m/s) and NIST J. Res. 1972 measurement (tf.nist.gov/general/pdf/527.pdf)
- APS News July 2010, Fizeau (Galileo lanterns; Roemer 1676; Fizeau 1849, 313 300 km/s, about 5% high)
- Wikipedia Fizeau's measurement (8633 m, 720 notches, 25.2 turns per second -> 313 274 304 m/s, 4.5% high) and Speed of light (Galileo proposal 1638; Foucault 1862 298 000 ± 500 km/s, −0.60%; Michelson 1926 299 796 ± 4 km/s)
- Baez and DESY "How is the speed of light measured?" (same table)
- NASA Moon Fact Sheet (mean distance 384 400 km)
- IAU 2012 astronomical unit 149 597 870 700 m.
Checked: 2026-10-17