Q.What should be the distance between the object in Exercise 9.23 and the magnifying glass if the virtual image of each square in the figure is to have an area of 6.25 mm2. Would you be able to see the squares distinctly with your eyes very close to the magnifier?
[Note: Exercises 9.22 to 9.24 will help you clearly understand the difference between magnification in absolute size and the angular magnification (or magnifying power) of an instrument.]
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🔒 Start your 14-day free trial to unlock the full solution →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 (fo), which forms a real, inverted, magnified image inside the tube.
- That real image falls just inside the focus of the eyepiece (fe), which acts as a simple magnifier, producing a large virtual, magnified final image for the eye.
Because each stage magnifies, the effects multiply:
M=mo×me
The objective's magnification
mo=uovo≈foL
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 fo, 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 cm, largest magnification):
me=1+feD
- Final image at infinity (relaxed eye, "normal adjustment"):
me=feD
Total magnifying power
Image at the near point: M=foL(1+feD)
Image at infinity: M=foL⋅feD
High magnification needs short fo and fe (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 fo=1.0 cm, eyepiece fe=2.5 cm, tube length L=20 cm, near point D=25 cm. Find M with the final image at the near point.
mo=1.020=20,me=1+2.525=11
M=20×11=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=Mo×Me=(foL)×(feD)
Where:
- fo = focal length of objective
- fe = 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 Mo
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 (fo).
Step 2: Using the lens formula
For a thin lens:
vo1−uo1=fo1
(Using sign convention: uo is negative, vo is positive)
Step 3: The tube length approximation
In a standard microscope, the specimen is placed very close to fo, so:
- uo≈−fo (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:
vo≈fo+L
Step 4: Magnification formula
Lateral magnification by objective:
Mo=∣uo∣vo≈fofo+L=1+foL
Since L≫fo in practice, 1 is negligible:
Mo≈foL
Why this makes sense: A shorter fo 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 Me
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:
Me=angle subtended by object at near pointangle subtended by image at eye
For a simple magnifier with image at infinity:
Me=feD
Where D=25 cm (standard near point). …
Each small square on the card has side 1 mm and the magnifying glass has focal length f=9 cm (carried over from the previous exercise).
Required magnification. The virtual image of a square must have area 6.25 mm2, so its side is 6.25=2.5 mm and the linear magnification is
m=1 mm2.5 mm=2.5
Object distance. For an erect virtual image v=mu=2.5u. The lens formula v1−u1=f1 gives
2.5u1−u1=91⇒u−0.6=91⇒u=−5.4 cm
so the object is 5.4 cm from the lens and the image is at v=2.5×(−5.4)=−13.5 cm. …
Place the object 5.4 cm from the lens; the image then forms 13.5 cm away. No, the squares cannot be seen distinctly because 13.5 cm is inside the 25 cm near point.
Data
From the earlier exercise, each square has side 1 mm and the magnifying glass (converging lens) has focal length f=9 cm.
Step 1 — Magnification needed for the required image area
The virtual image of each square must have area 6.25 mm2, so the image side is
6.25 mm2=2.5 mm
The linear magnification is therefore
m=object sideimage side=1 mm2.5 mm=2.5
Step 2 — Object distance from the lens formula
For an erect virtual image the magnification is m=v/u, so v=2.5u. Substituting into v1−u1=f1:
2.5u1−u1=91
2.5u1−2.5=91⇒2.5u−1.5=91⇒u−0.6=91
u=−0.6×9=−5.4 cm
The object is 5.4 cm in front of the lens — inside f=9 cm, which correctly gives a virtual image.
Step 3 — Image position
v=2.5u=2.5×(−5.4 cm)=−13.5 cm …
Method: Thin Lens Formula with Magnification for a Virtual Image
This problem uses the thin lens equation combined with linear magnification to find the object distance when the image size is specified.
Steps
-
Identify given data
- Lens focal length: f=10 cm (from Exercise 9.23 context)
- Original square side length: a=1 mm (from figure in Exercise 9.23)
- Required virtual image area: Ai=6.25 mm2
- Therefore, image side length: ai=6.25=2.5 mm
-
Calculate required linear magnification
Linear magnification m=object sizeimage size=1 mm2.5 mm=2.5
-
Apply magnification formula for a lens
For a thin lens: m=uv
Since the image is virtual and upright, m is positive:
v=mu=2.5u
- Use thin lens equation
f1=v1−u1
(Note: sign convention — for virtual image, v is negative if using real-is-positive; but here we use magnitudes with sign awareness)
Substituting v=−2.5u (virtual image on same side as object):
101=−2.5u1−u1
101=−2.5u1−u1=−u1(2.51+1)=−u1×1.4
u=−14 cm …
Common Mistakes: Microscope Magnification (Exercise 9.23)
Mistake 1: Confusing Linear Magnification with Angular Magnification
The error: Students often use the formula for angular magnification (M=D/f) directly to find the image distance or object distance, when the problem actually asks about absolute size magnification (linear magnification).
Why it's wrong: The question asks for the image to have an area of 6.25 mm2. This is about linear magnification m=hohi, not angular magnification. The two are fundamentally different:
- Linear magnification m=uv (absolute size change)
- Angular magnification M=fD (apparent size change when eye is relaxed)
How to avoid: Read carefully — if the problem gives actual dimensions of the image (like area), use linear magnification. If it asks about "magnifying power" or "angular magnification," use the angle-based formula.
Mistake 2: Forgetting to Take Square Root for Area-to-Length Conversion
The error: Students treat the area 6.25 mm2 as if it were a linear dimension, plugging it directly into magnification formulas.
Why it's wrong: Magnification is defined for linear dimensions (length, height), not area. If the image area is 6.25 mm2, the linear magnification factor is:
m=object side lengthimage side length=object side length6.25=object side length2.5 mm
How to avoid: Always convert area to linear dimension by taking the square root before using any magnification formula.
Mistake 3: Using the Wrong Sign Convention for Virtual Image
The error: Students treat the image distance v as positive when using the lens formula f1=v1−u1.
Why it's wrong: For a magnifying glass (convex lens used as a simple microscope), the image is virtual and on the same side as the object. According to the Cartesian sign convention:
- v is negative for virtual images
- u is negative (object on left side)
The correct lens formula becomes:
f1=v1−u1
where both u and v are negative.
How to avoid: Draw a ray diagram first. If the image is on the same side as the object, v is negative. Always write the sign convention at the top of your solution.
Mistake 4: Assuming the Image is at Infinity (Relaxed Eye)
The error: Students automatically set v=∞ (image at infinity) because that's the "normal" adjustment for a magnifying glass. …
- JKBOSE Class 12 Annual Regular Examination 2026Set SZ1 markMCQQ.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 fo 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).
…
- JKBOSE Class 12 Annual Regular Examination 2025Set SZ1 markMCQQ.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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