A person with a normal near point ($25\ \text{cm}$) using a compound microscope with objective of focal length $8.0\ \text{mm}$ and an eyepiece of focal length $2.5\ \text{cm}$ can bring an object placed at $9.0\ \text{mm}$ from the objective in sharp focus. What is the separation between the two lenses? Calculate the magnifying power of the microscope.

A person with a normal near point (25cm) using a compound microscope with objective of focal length 8.0mm and

Exercises · 9.12

25\ \text{cm}

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Concept understanding — Microscope Magnification

Microscope Magnification

A compound microscope views very small, nearby objects using two lenses in sequence: the objective (near the object) and the eyepiece (near the eye). Its total magnifying power is the product of what each lens contributes.

How the two lenses work together

The object sits just beyond the focus of the short-focal-length objective ( $f_o$ ), which forms a real, inverted, magnified image inside the tube.
That real image falls just inside the focus of the eyepiece ( $f_e$ ), which acts as a simple magnifier, producing a large virtual, magnified final image for the eye.

Because each stage magnifies, the effects multiply:

M = m_o \times m_e

The objective's magnification

m_o = \frac{v_o}{u_o} \approx \frac{L}{f_o}

where $L$ is the tube length (roughly the distance between the objective's second focal point and the eyepiece's first focal point). The object sits close to $f_o$ , so this approximation holds for a well-designed microscope.

The eyepiece's magnification

The eyepiece behaves as a simple magnifier:

Final image at the near point ( $D = 25\ \text{cm}$ , largest magnification):

m_e = 1 + \frac{D}{f_e}

Final image at infinity (relaxed eye, "normal adjustment"):

m_e = \frac{D}{f_e}

Total magnifying power

M = \frac{L}{f_o}\left(1 + \frac{D}{f_e}\right)

Important

High magnification needs short $f_o$ and $f_e$ (both sit in denominators) and a large tube length $L$ — this is why a microscope objective is always a very short-focus lens.

Worked example

Objective $f_o = 1.0\ \text{cm}$ , eyepiece $f_e = 2.5\ \text{cm}$ , tube length $L = 20\ \text{cm}$ , near point $D = 25\ \text{cm}$ . Find $M$ with the final image at the near point.

m_o = \frac{20}{1.0} = 20, \qquad m_e = 1 + \frac{25}{2.5} = 11

$M = 20 \times 11 = 220$ …

Why this formula?

Microscope Magnification: Why the Formula Holds

Let's build the understanding from first principles — not just memorizing formulas, but seeing why they work.

1. What Does "Magnification" Mean in a Microscope?

A microscope creates a larger apparent image of a tiny object. The total magnification is the product of two stages:

Objective lens — creates a real, enlarged, inverted image of the specimen.
Eyepiece (ocular) — acts as a simple magnifier to view that real image.

So:

Total magnification = (magnification by objective) × (magnification by eyepiece)

2. The Key Formula

For a compound microscope in normal adjustment (final image at infinity, relaxed eye):

M = M_o \times M_e = \left( \frac{L}{f_o} \right) \times \left( \frac{D}{f_e} \right)

Where:

$f_o$ = focal length of objective
$f_e$ = focal length of eyepiece
$L$ = tube length (distance between second focal point of objective and first focal point of eyepiece)
$D$ = near point distance of the eye (usually 25 cm)

3. Derivation of Objective Magnification $M_o$

Step 1: How the objective works

The objective lens forms a real, inverted, enlarged image of the specimen. The specimen is placed just outside its focal point ( $f_o$ ).

Step 2: Using the lens formula

For a thin lens:

\frac{1}{v_o} - \frac{1}{u_o} = \frac{1}{f_o}

(Using sign convention: $u_o$ is negative, $v_o$ is positive)

Step 3: The tube length approximation

In a standard microscope, the specimen is placed very close to $f_o$ , so:

$u_o \approx -f_o$ (object just beyond focal point)
The image is formed at the first focal point of the eyepiece, which is at a distance $L$ from the second focal point of the objective.

Thus:

v_o \approx f_o + L

Step 4: Magnification formula

Lateral magnification by objective:

M_o = \frac{v_o}{|u_o|} \approx \frac{f_o + L}{f_o} = 1 + \frac{L}{f_o}

Since $L \gg f_o$ in practice, $1$ is negligible:

\boxed{M_o \approx \frac{L}{f_o}}

Why this makes sense: A shorter $f_o$ means the objective is more "powerful" — it bends light more sharply, creating a larger image at the fixed tube length.

4. Derivation of Eyepiece Magnification $M_e$

Step 1: The eyepiece as a simple magnifier

The eyepiece takes the real image from the objective and acts like a magnifying glass. For relaxed eye (final image at infinity), the real image must be placed at the focal point of the eyepiece.

Step 2: Angular magnification

Angular magnification is defined as:

M_e = \frac{\text{angle subtended by image at eye}}{\text{angle subtended by object at near point}}

For a simple magnifier with image at infinity:

M_e = \frac{D}{f_e}

Where $D = 25$ cm (standard near point). …

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The objective forms a real image $v_o=7.2\ \text{cm}$ from itself; the eyepiece needs its object at $u_e\approx-2.27\ \text{cm}$ to place the final image at the near point. The lens separation is $v_o+|u_e|\approx9.47\ \text{cm}$ , and the magnifying power is $M=m_o\times m_e=-88$ (magnitude 88; the negative sign shows the final image is inverted).

Step 1 — image formed by the objective

$f_o=8.0\ \text{mm}=0.8\ \text{cm}$ , $u_o=-0.9\ \text{cm}$ (object $9.0\ \text{mm}$ in front, negative by sign convention).

\frac{1}{v_o}-\frac{1}{u_o}=\frac{1}{f_o} \;\Rightarrow\; \frac{1}{v_o}=\frac{1}{0.8}-\frac{1}{0.9}=\frac{0.9-0.8}{0.72}=\frac{0.1}{0.72}

v_o = 7.2\ \text{cm}

Step 2 — object distance for the eyepiece

For the final image at the near point, $v_e=-25\ \text{cm}$ , $f_e=2.5\ \text{cm}$ .

\frac{1}{v_e}-\frac{1}{u_e}=\frac{1}{f_e} \;\Rightarrow\; -\frac{1}{u_e}=\frac{1}{f_e}-\frac{1}{v_e}=\frac{1}{2.5}+\frac{1}{25}=\frac{11}{25}

u_e = -\frac{25}{11} \approx -2.27\ \text{cm}

Step 3 — separation between the lenses

The intermediate image lies $v_o=7.2\ \text{cm}$ from the objective and $|u_e|\approx2.27\ \text{cm}$ from the eyepiece, on the same point between the two lenses, so

L = v_o + |u_e| = 7.2+2.27 = 9.47\ \text{cm}

Step 4 — magnifying power

$m_o = \frac{v_o}{u_o} = \frac{7.2}{-0.9} = -8$ …

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Method: Two-Lens Image Formation (Compound Microscope Analysis)

This problem uses the compound microscope as two successive lens systems — the objective forms a real, inverted image, which then acts as the object for the eyepiece.

Step 1: Understand the given data

Quantity	Value
Near point ( $D$ )	$25\ \text{cm}$
Objective focal length ( $f_o$ )	$8.0\ \text{mm} = 0.8\ \text{cm}$
Eyepiece focal length ( $f_e$ )	$2.5\ \text{cm}$
Object distance from objective ( $u_o$ )	$9.0\ \text{mm} = 0.9\ \text{cm}$

Step 2: Find the image distance for the objective

Use the lens formula for the objective:

\frac{1}{v_o} - \frac{1}{u_o} = \frac{1}{f_o}

Sign convention: For a real object, $u_o$ is negative.

\frac{1}{v_o} - \frac{1}{(-0.9)} = \frac{1}{0.8}

\frac{1}{v_o} + \frac{1}{0.9} = \frac{1}{0.8}

\frac{1}{v_o} = \frac{1}{0.8} - \frac{1}{0.9} = \frac{0.9 - 0.8}{0.72} = \frac{0.1}{0.72}

v_o = \frac{0.72}{0.1} = 7.2\ \text{cm}

The objective forms a real image at $7.2\ \text{cm}$ on the other side.

Step 3: Find the separation between lenses

The eyepiece is adjusted so that the final image is at the near point ( $25\ \text{cm}$ from the eye) for maximum magnification.

For the eyepiece:

Final image distance ( $v_e$ ) = $-25\ \text{cm}$ (virtual image, on same side as object)
$f_e = 2.5\ \text{cm}$

Using lens formula for eyepiece:

\frac{1}{v_e} - \frac{1}{u_e} = \frac{1}{f_e}

\frac{1}{(-25)} - \frac{1}{u_e} = \frac{1}{2.5}

-\frac{1}{25} - \frac{1}{u_e} = \frac{1}{2.5}

- \frac{1}{u_e} = \frac{1}{2.5} + \frac{1}{25} = \frac{10}{25} + \frac{1}{25} = \frac{11}{25}

u_e = -\frac{25}{11} \approx -2.27\ \text{cm}

The negative sign means the object for the eyepiece is inside its focal length — as expected.

Separation between lenses = $v_o + |u_e|$ …

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Common Mistakes & How to Avoid Them

Mistake 1: Confusing the two magnifications

Students often mix up magnifying power of the eyepiece ( $m_e$ ) with magnification of the objective ( $m_o$ ), or use the wrong formula for each.

How to avoid:

Objective magnification is always:

m_o = -\frac{v_o}{u_o}

where $v_o$ = image distance from objective, $u_o$ = object distance from objective.

Eyepiece magnification depends on final image condition:
- For final image at infinity (relaxed eye):

m_e = \frac{D}{f_e} \quad \text{(where } D = 25\ \text{cm)}

For final image at near point (maximum magnification):

m_e = 1 + \frac{D}{f_e}

Key insight: The problem says "sharp focus" — this usually means the final image is formed at the near point (25 cm), so use $m_e = 1 + \frac{D}{f_e}$ .

Mistake 2: Forgetting the sign convention

Students often ignore the negative sign in $m_o = -v_o/u_o$ , leading to wrong total magnification.

How to avoid:

The negative sign indicates the image is inverted relative to the object.
For total magnifying power, we take absolute values:

M = |m_o| \times m_e

Always write the sign first, then take magnitude for the final answer.

Mistake 3: Using the wrong lens formula for the objective

Students sometimes plug $u_o = 9.0\ \text{mm}$ directly into the lens formula without checking if it's beyond the focal length.

How to avoid:

For a real, enlarged image in a microscope, the object must be placed just beyond $f_o$ .
Here: $f_o = 8.0\ \text{mm}$ , $u_o = 9.0\ \text{mm}$ → valid (object is beyond focal point).
Use the lens formula correctly:

\frac{1}{v_o} - \frac{1}{u_o} = \frac{1}{f_o}

with sign convention: $u_o$ is negative (real object on left), $f_o$ positive (convex lens).

Mistake 4: Mixing units (mm vs cm)

The objective focal length is in mm, the eyepiece focal length is in cm — students often forget to convert.

How to avoid:

Convert everything to the same unit before calculating.
Best practice: Convert to cm (since near point $D = 25\ \text{cm}$ $D = 25 cm$ ):
- $f_o = 8.0\ \text{mm} = 0.8\ \text{cm}$
- $u_o = 9.0\ \text{mm} = 0.9\ \text{cm}$
- $f_e = 2.5\ \text{cm}$ (already in cm)

Mistake 5: Confusing "separation between lenses" with image distances

Students sometimes think the lens separation is simply $v_o + v_e$ , but forget that $v_e$ is measured from the eyepiece, not from the objective.

How to avoid:

Lens separation $L$ = distance from objective to eyepiece = $v_o + u_e$ where $u_e$ is the object distance for the eyepiece (the intermediate image formed by the objective). …

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Same / Similar Concept — real previous-year questions on the same or a closely similar concept, not this exact question.

JKBOSE Class 12 Annual Regular Examination 2026Set SZ1 markMCQ
$Q. The image formed by the objective of a compound microscope is$
(a) Real, inverted
(b) Virtual, erect
(c) Virtual, inverted
(d) Real, erect
›Reveal solutionSolution

In a compound microscope, the tiny object is placed just beyond the focal length of the objective lens, so the objective forms a real, inverted, and magnified image — this image then serves as the object for the eyepiece.

Concept. A compound microscope has two converging lenses: the objective (short focal length, faces the object) and the eyepiece (the one the observer looks through).

Objective's job. The object is placed slightly outside the focal length $f_o$ of the objective. For a convex lens with the object placed just beyond $f$ , the image formed is real, inverted, and magnified — this is the same ray behaviour as a convex lens forming a real image when the object lies between $f$ and $2f$ (or just beyond $f$ ).

…

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JKBOSE Class 12 Annual Regular Examination 2025Set SZ1 markMCQ
$Q. In a compound microscope, the distance between objective lens and eye lens is : (A) Fixed (B) Variable (C) Infinite (D) 1 metre$
›Reveal solutionSolution

The distance between the objective lens and the eye lens (eyepiece) of a compound microscope is variable, because it must be adjusted for focusing.

In a compound microscope, the object is placed just beyond the focal length of the objective lens, which forms a real, inverted, magnified image. This image acts as the object for the eyepiece, which further magnifies it to form a final virtual image (usually at the near point or at infinity, for least eye strain).

…

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Step 1 — image formed by the objective

Step 2 — object distance for the eyepiece

Step 3 — separation between the lenses

Step 4 — magnifying power

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