AP Unit 13 Problems
11 learning problems for Unit 13. Draw the situation, name the model and explain why each step follows. These are authored practice, with worked solutions on a separate page.
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Problem 1
A laser beam travels through air toward a large flat mirror. Before reflection, its wavefronts are vertical parallel lines and move rightward.
Part a
Draw or describe the incident rays relative to the wavefronts. Specify arrows and explain why the ray model is suitable here.
Part b
The same coherent, approximately monochromatic laser is redirected through a slit comparable to its wavelength and forms bright and dark bands on a screen. State what coherent and monochromatic mean, explain which source properties remain, and explain why rays alone fail to predict the bands.
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Problem 2
Three parallel rays strike a horizontal flat reflecting surface at 40.0° to the surface. The surface is then replaced by a rough sheet with tiny patches tilted differently.
Part a
Find the incidence and reflection angles for the flat surface and draw an arrowed incident/reflected pair with a normal.
Part b
Compare the reflected bundles from the smooth flat surface and rough sheet. Explain in terms of normals whether the law still holds.
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Problem 3
A 2.00 cm object is 30.0 cm in front of a concave spherical mirror of radius 40.0 cm. Use the real-is-positive convention.
Part a
Find f, d_i, magnification, and signed image height; classify the image.
Part b
Construct the three principal rays to locate the image tip. Clearly distinguish the vertex ray from a center-of-curvature ray.
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Problem 4
Compare a plane mirror, a convex mirror with f = −12.0 cm, and a concave mirror with f = +12.0 cm. Each has the same upright real object 6.00 cm in front.
Part a
Calculate signed image distances and magnifications for all three mirrors. Create a comparison table including focal length, d_i, m, real/virtual type, orientation, relative size, and physical image side.
Part b
Describe the convex mirror’s parallel-ray behavior and the backward-extension construction. Could a screen behind the mirror receive its image?
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Problem 5
A beam with vacuum wavelength 540 nm enters glass (n = 1.60) from air (n = 1.00). The beam makes 55.0° with the flat glass surface.
Part a
Find the incidence angle to the normal, transmitted angle, speed, and wavelength in glass. State whether frequency changes.
Part b
If the incoming beam is changed to normal incidence, compare its direction, speed, and wavelength in the glass with those of the original transmitted beam.
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Problem 6
A transparent block has n = 1.50 and is surrounded by air, n = 1.00. Light inside it strikes a flat face.
Part a
Derive the critical-angle expression from Snell’s law and calculate it.
Part b
For incident angles 30.0°, θ_c, and 50.0°, draw or describe transmitted and reflected paths in the ideal model.
Part c
A student predicts the same critical angle for air-to-block travel. Evaluate the claim.
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Problem 7
A thin converging lens in air has f = +10.0 cm. A 1.50 cm tall object is 25.0 cm to its left, with light traveling left to right.
Part a
Find image position, magnification, and signed height. State screen placement and image description.
Part b
Construct the image with the three principal rays. Mark both focal points and identify which focus each relevant ray uses.
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Problem 8
Compare a diverging lens with f = −12.0 cm and a converging lens with f = +12.0 cm. Each has a real object 8.00 cm away in air.
Part a
Find both image distances and magnifications. Explain why both images are virtual but differ in size.
Part b
Describe the diverging-lens parallel ray and center ray, including backward extensions. Describe a third principal ray as a check.
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Problem 9
Students use a ray box, protractor, paper, and a semicircular transparent block to measure refraction. They find air angles 20.0°, 40.0°, and 60.0° paired with block angles 13.2°, 25.4°, and 35.3°, all measured to the normal at the flat face.
Part a
Design a procedure that changes the incident angle while keeping the material, flat-face entry or exit point, and unwanted curved-face refraction controlled. Explain why passage normal to the curved face prevents unwanted directional bending. State how you would also check reflection at the flat face.
Part b
Choose a sine transformation that makes the refraction data linear, then construct the quantitative graph using all three data pairs. Label both axes as dimensionless sine values, show numerical scales and points, and draw a best-fit line. Use its slope to estimate the block index. Discuss why very small angles can be poor measurements.
Part c
How could the same block test a critical-angle prediction? Give the required travel direction and observations at and above the prediction.
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Problem 10
A concave mirror and a thin converging lens each have f = +15.0 cm, with a real object 30.0 cm in front or on the incident side. A convex mirror and a thin diverging lens each have f = −15.0 cm with the same real-object distance.
Part a
Create a comparison table with one row for each system and columns for f, d_i, m, real/virtual type, orientation, relative size, and physical side. Explain why equal algebraic results can locate images on different physical sides.
Part b
Describe how the vertex/center principal ray differs for a mirror and a thin lens, and how the parallel principal ray behaves in each converging system.
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Problem 11
Students project a bright object through a thin converging lens onto a screen. Their (d_o, d_i) data in centimeters are (18.0, 36.0), (24.0, 24.0), and (36.0, 18.0).
Part a
Derive a linear graph form by rearranging the thin-lens equation. Construct a quantitative reciprocal-distance graph using all three data pairs, with labeled axes, units, numerical scales, plotted points, and a fit line. Use its slope and intercept to estimate focal length and check the model. Explain why the screen images are real.
Part b
State a hands-on procedure for collecting such data and estimating uncertainty. Predict the image when d_o is changed to 8.00 cm and explain how to observe it.
Part c
The center ray is modeled as straight, although refraction occurs at a lens’s surfaces. Explain this approximation and name a change that would make a simple thin-lens construction less reliable.
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More chapter problems
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Require the reflected rays to agree
A concave spherical mirror has nonnegative radius of curvature R = 24.0 cm. A real upright object 2.00 cm tall is 18.0 cm in front. Use the paraxial approximation and the real-is-positive convention.
(a) Determine signed f, dᵢ, m, and hᵢ. State the physical image side, real/virtual type, orientation, and size relative to the object.
(b) Construct a scaled, arrowed three-principal-ray diagram from the object tip. Mark the vertex, focus, curvature center, and image. Show the parallel ray, the vertex ray, and the focal ray; explain how the actual reflected intersection establishes image type and how its height checks part (a).
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Worked solution and rubric →Revisit the explanation →Revisit the explanation →Read the relevant lesson →
A screen image and an apparent image from the same lens
A thin converging lens in air has f = +12.0 cm with the same medium on both sides. Light travels left to right from an upright 2.00 cm object. First dₒ = +30.0 cm; then the object is moved to dₒ = +8.00 cm. Use real-is-positive optical distances.
(a) For the 30.0 cm object position, calculate dᵢ, m, and hᵢ and construct an arrowed three-principal-ray diagram marking both foci. Determine image side, type, orientation and size, and say where a screen should go. Explain how the actual rays justify the type.
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(b) For the 8.00 cm object position, calculate dᵢ, m, and hᵢ and construct all three principal rays again. Distinguish solid actual transmitted paths from dashed backward extensions. Use the diagram to classify the image and explain how an observer can see it despite the failure of a screen on the image side.
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Worked solution and rubric →Revisit the explanation →Revisit the explanation →Read the relevant lesson →