Virtual laboratory/Physics/Optics/Converging lens — where will the image form?

Converging lens — where will the image form?

What we will do: We will slide an object in front of a converging lens and check where the image forms and what kind it is — larger or smaller, upright or inverted.

What you see on screen: The optical axis with the lens, the focal points F and 2F, an arrow-object and the three principal rays that intersect at the image; sliders for the focal length and the object distance. For a virtual image the rays are extended backward with dashed lines. Readouts: focal length, the distances x and y, magnification, and the type and orientation of the image.

Converging lens — where will the image form?
Physics · Optics · Lenses (FIZ.FALE.PR.16)
The object stands far in front of the lens (farther than 2f). The image will be:
focal len. f
10 cm
object x
30 cm
image y
15.0 cm
magnif.
0.50×
image
real, inverted
🎯 Challenge: place the object so the lens acts as the given device

What just happened?

An object far in front of the lens produced a smaller image, flipped upside down. That is how a camera and your eye work — the image on the retina is inverted too (the brain “flips” it back).

How the lens forms the image — three rays:

• parallel to the axis → refracts through the focal point FF, • through the center of the lens → straight through, no bending, • through the front focal point → onward parallel to the axis. Where they cross — there is the image.

Lens equation:

1f=1x+1yy=x fx−f\dfrac{1}{f} = \dfrac{1}{x} + \dfrac{1}{y} \qquad y = \dfrac{x\,f}{x - f}

ff — focal length, xx — object distance, yy — image distance.

How large is the image? Magnification:

p=yxp = \dfrac{y}{x}

p>1p > 1 enlarged, p<1p < 1 reduced.

Everything depends on where you place the object:

farther than 2f → real, inverted, reduced (camera and eye), between f and 2f → real, inverted, enlarged (projector), closer than f → virtual, upright, enlarged, on the same side (magnifier).

The limiting point x = f:

After the lens the rays run parallel and never meet — the image escapes to infinity. That is why a zero appears in the denominator x−fx - f.

Why you need this for the exam:

The equation 1f=1x+1y\tfrac{1}{f}=\tfrac{1}{x}+\tfrac{1}{y} plus the sign of the result (y>0y>0 real, y<0y<0 virtual) solves every lens problem. The rest is the construction of the three rays.

Remember: the same lens is a camera, a projector, or a magnifier — depending only on whether the object stands farther than 2f, between f and 2f, or closer than f.

Geometric construction · NexTutor Virtual laboratory

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Theory & formulas

The lens equation

The position of the image is related to the position of the object by the equation: 1f=1x+1y\dfrac{1}{f} = \dfrac{1}{x} + \dfrac{1}{y}

Magnification

The ratio of the image height to the object height: p=yxp = \dfrac{y}{x} p>1p>1 — the image is enlarged, p<1p<1 — reduced.

Type of image

  • object farther than the focal point (x>fx>f): a real and inverted image (it can be projected on a screen),
  • object closer than the focal point (x<fx<f): a virtual image, upright and enlarged — the lens acts as a magnifier.

Notation: ff — focal length (positive for a converging lens), xx — object distance, yy — image distance, pp — magnification.

Frequently asked questions

›

What is the lens equation?

1/f = 1/x + 1/y, where f is the focal length, x is the object distance and y is the image distance.

›

When does a lens give a real image and when a virtual one?

Real when the object is farther than the focal point (x > f); virtual and enlarged when it is closer (x < f) — then it acts as a magnifier.

›

How do you calculate the magnification of the image?

p = y/x (or h'/h); p > 1 means enlargement, p < 1 means reduction.

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