Practice worksheet for drawing ray diagrams and determining image characteristics for convex lenses.
Convex Lenses Practice Worksheet with three problems involving object placement and ray diagrams for convex lenses.
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Show Answer Key & Explanations
Step-by-step solution for: 10.14 PT Convex Lens Practice | PDF | Lens (Optics) | Optical Devices
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Show Answer Key & Explanations
Step-by-step solution for: 10.14 PT Convex Lens Practice | PDF | Lens (Optics) | Optical Devices
Let's solve each problem step by step using the principles of convex lens imaging. We’ll use the lens formula and ray diagram rules to determine the image characteristics: location, direction (orientation), size, and type (real or virtual).
---
- Focal length (f) = 15.0 cm for all lenses (convex)
- Object distance (do) is given in each case
- Use lens formula:
$$
\frac{1}{f} = \frac{1}{d_o} + \frac{1}{d_i}
$$
where:
- $ f $ = focal length
- $ d_o $ = object distance
- $ d_i $ = image distance
We'll also use ray tracing rules:
1. A ray parallel to the principal axis passes through the focal point after refraction.
2. A ray through the center of the lens continues straight.
3. A ray through the focal point emerges parallel to the axis.
Image properties depend on object position relative to F and 2F:
- Beyond 2F: Real, inverted, reduced
- At 2F: Real, inverted, same size
- Between F and 2F: Real, inverted, enlarged
- At F: No image (rays parallel)
- Between F and lens: Virtual, upright, enlarged
---
## ✔ Problem 1:
> A 15.0 cm object is placed 60.0 cm from a convex lens with focal length 15.0 cm.
- $ d_o = 60.0 $ cm
- $ f = 15.0 $ cm
$$
\frac{1}{d_i} = \frac{1}{f} - \frac{1}{d_o} = \frac{1}{15} - \frac{1}{60}
= \frac{4 - 1}{60} = \frac{3}{60} = \frac{1}{20}
\Rightarrow d_i = 20.0 \text{ cm}
$$
So image is 20.0 cm on the opposite side of the lens.
- Object is at 60 cm, which is beyond 2F (since 2F = 30 cm).
- So image should be:
- Real (on opposite side)
- Inverted
- Reduced (smaller than object)
$$
m = -\frac{d_i}{d_o} = -\frac{20}{60} = -\frac{1}{3}
$$
Negative → inverted; magnitude < 1 → reduced
| Location | Between F and 2F (on other side) |
|----------------|----------------------------------|
| Direction | Inverted |
| Size | Reduced |
| Type | Real |
✔ Answer: Image is real, inverted, reduced, located between F and 2F on the opposite side.
---
## ✔ Problem 2:
> A 15.0 cm object is placed 30.0 cm from a convex lens with focal length 15.0 cm.
- $ d_o = 30.0 $ cm
- $ f = 15.0 $ cm
$$
\frac{1}{d_i} = \frac{1}{15} - \frac{1}{30} = \frac{2 - 1}{30} = \frac{1}{30}
\Rightarrow d_i = 30.0 \text{ cm}
$$
- Object is at 30 cm, which is exactly at 2F (since 2F = 30 cm)
- Image is also at 2F on the other side
- Image is:
- Real
- Inverted
- Same size as object
Magnification:
$$
m = -\frac{30}{30} = -1
$$
→ Inverted, same size
| Location | At 2F (on other side) |
|----------------|----------------------------------|
| Direction | Inverted |
| Size | Same size |
| Type | Real |
✔ Answer: Image is real, inverted, same size, located at 2F on the opposite side.
---
## ✔ Problem 3:
> A 15.0 cm object is placed 16.0 cm from a convex lens with focal length 15.0 cm.
- $ d_o = 16.0 $ cm
- $ f = 15.0 $ cm
$$
\frac{1}{d_i} = \frac{1}{15} - \frac{1}{16} = \frac{16 - 15}{240} = \frac{1}{240}
\Rightarrow d_i = 240 \text{ cm}
$$
Wait — that’s positive? Let’s double-check:
$$
\frac{1}{d_i} = \frac{1}{15} - \frac{1}{16} = \frac{16 - 15}{240} = \frac{1}{240} \Rightarrow d_i = 240 \text{ cm}
$$
Yes, positive → real image?
But wait! Object is between F and 2F? Let’s check:
- F = 15 cm, 2F = 30 cm
- Object at 16 cm → between F and 2F
So we expect a real, inverted, enlarged image beyond 2F.
And yes, $ d_i = 240 $ cm → far beyond 2F.
$$
m = -\frac{d_i}{d_o} = -\frac{240}{16} = -15
$$
→ Highly enlarged, inverted
| Location | Beyond 2F (on other side) |
|----------------|----------------------------------|
| Direction | Inverted |
| Size | Enlarged |
| Type | Real |
✔ Answer: Image is real, inverted, enlarged, located beyond 2F on the opposite side.
---
## 📐 Ray Diagrams (Summary):
For each case, draw three rays from the top of the object:
1. Parallel to axis → refracts through F
2. Through center → straight line
3. Through F → refracts parallel
The intersection point gives the image.
- Rays converge between F and 2F → smaller inverted image
- Rays converge at 2F → same size, inverted
- Rays converge beyond 2F → larger, inverted image
---
## ✔ Final Answers:
| Location | Between F and 2F (on other side) |
|----------------|----------------------------------|
| Direction | Inverted |
| Size | Reduced |
| Type | Real |
| Location | At 2F (on other side) |
|----------------|----------------------------------|
| Direction | Inverted |
| Size | Same size |
| Type | Real |
| Location | Beyond 2F (on other side) |
|----------------|----------------------------------|
| Direction | Inverted |
| Size | Enlarged |
| Type | Real |
---
Let me know if you'd like hand-drawn ray diagrams sketched out or explained further!
---
🔍 Key Concepts:
- Focal length (f) = 15.0 cm for all lenses (convex)
- Object distance (do) is given in each case
- Use lens formula:
$$
\frac{1}{f} = \frac{1}{d_o} + \frac{1}{d_i}
$$
where:
- $ f $ = focal length
- $ d_o $ = object distance
- $ d_i $ = image distance
We'll also use ray tracing rules:
1. A ray parallel to the principal axis passes through the focal point after refraction.
2. A ray through the center of the lens continues straight.
3. A ray through the focal point emerges parallel to the axis.
Image properties depend on object position relative to F and 2F:
- Beyond 2F: Real, inverted, reduced
- At 2F: Real, inverted, same size
- Between F and 2F: Real, inverted, enlarged
- At F: No image (rays parallel)
- Between F and lens: Virtual, upright, enlarged
---
## ✔ Problem 1:
> A 15.0 cm object is placed 60.0 cm from a convex lens with focal length 15.0 cm.
Given:
- $ d_o = 60.0 $ cm
- $ f = 15.0 $ cm
Step 1: Use lens formula
$$
\frac{1}{d_i} = \frac{1}{f} - \frac{1}{d_o} = \frac{1}{15} - \frac{1}{60}
= \frac{4 - 1}{60} = \frac{3}{60} = \frac{1}{20}
\Rightarrow d_i = 20.0 \text{ cm}
$$
So image is 20.0 cm on the opposite side of the lens.
Step 2: Analyze:
- Object is at 60 cm, which is beyond 2F (since 2F = 30 cm).
- So image should be:
- Real (on opposite side)
- Inverted
- Reduced (smaller than object)
Magnification:
$$
m = -\frac{d_i}{d_o} = -\frac{20}{60} = -\frac{1}{3}
$$
Negative → inverted; magnitude < 1 → reduced
Fill in table:
| Location | Between F and 2F (on other side) |
|----------------|----------------------------------|
| Direction | Inverted |
| Size | Reduced |
| Type | Real |
✔ Answer: Image is real, inverted, reduced, located between F and 2F on the opposite side.
---
## ✔ Problem 2:
> A 15.0 cm object is placed 30.0 cm from a convex lens with focal length 15.0 cm.
Given:
- $ d_o = 30.0 $ cm
- $ f = 15.0 $ cm
Step 1: Lens formula
$$
\frac{1}{d_i} = \frac{1}{15} - \frac{1}{30} = \frac{2 - 1}{30} = \frac{1}{30}
\Rightarrow d_i = 30.0 \text{ cm}
$$
Step 2: Analyze:
- Object is at 30 cm, which is exactly at 2F (since 2F = 30 cm)
- Image is also at 2F on the other side
- Image is:
- Real
- Inverted
- Same size as object
Magnification:
$$
m = -\frac{30}{30} = -1
$$
→ Inverted, same size
Fill in table:
| Location | At 2F (on other side) |
|----------------|----------------------------------|
| Direction | Inverted |
| Size | Same size |
| Type | Real |
✔ Answer: Image is real, inverted, same size, located at 2F on the opposite side.
---
## ✔ Problem 3:
> A 15.0 cm object is placed 16.0 cm from a convex lens with focal length 15.0 cm.
Given:
- $ d_o = 16.0 $ cm
- $ f = 15.0 $ cm
Step 1: Lens formula
$$
\frac{1}{d_i} = \frac{1}{15} - \frac{1}{16} = \frac{16 - 15}{240} = \frac{1}{240}
\Rightarrow d_i = 240 \text{ cm}
$$
Wait — that’s positive? Let’s double-check:
$$
\frac{1}{d_i} = \frac{1}{15} - \frac{1}{16} = \frac{16 - 15}{240} = \frac{1}{240} \Rightarrow d_i = 240 \text{ cm}
$$
Yes, positive → real image?
But wait! Object is between F and 2F? Let’s check:
- F = 15 cm, 2F = 30 cm
- Object at 16 cm → between F and 2F
So we expect a real, inverted, enlarged image beyond 2F.
And yes, $ d_i = 240 $ cm → far beyond 2F.
Magnification:
$$
m = -\frac{d_i}{d_o} = -\frac{240}{16} = -15
$$
→ Highly enlarged, inverted
Fill in table:
| Location | Beyond 2F (on other side) |
|----------------|----------------------------------|
| Direction | Inverted |
| Size | Enlarged |
| Type | Real |
✔ Answer: Image is real, inverted, enlarged, located beyond 2F on the opposite side.
---
## 📐 Ray Diagrams (Summary):
For each case, draw three rays from the top of the object:
1. Parallel to axis → refracts through F
2. Through center → straight line
3. Through F → refracts parallel
The intersection point gives the image.
For Problem 1 (do = 60 cm):
- Rays converge between F and 2F → smaller inverted image
For Problem 2 (do = 30 cm):
- Rays converge at 2F → same size, inverted
For Problem 3 (do = 16 cm):
- Rays converge beyond 2F → larger, inverted image
---
## ✔ Final Answers:
Problem 1:
| Location | Between F and 2F (on other side) |
|----------------|----------------------------------|
| Direction | Inverted |
| Size | Reduced |
| Type | Real |
Problem 2:
| Location | At 2F (on other side) |
|----------------|----------------------------------|
| Direction | Inverted |
| Size | Same size |
| Type | Real |
Problem 3:
| Location | Beyond 2F (on other side) |
|----------------|----------------------------------|
| Direction | Inverted |
| Size | Enlarged |
| Type | Real |
---
Let me know if you'd like hand-drawn ray diagrams sketched out or explained further!
Parent Tip: Review the logic above to help your child master the concept of concave and convex lenses worksheet.