Refraction of Light, Total Internal Reflection, and Prisms

21 soru

Soru 1Soru

Which of the following conditions is necessary for total internal reflection to occur when light travels between two media?

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Cevap: Light must travel from an optically denser medium to an optically less dense medium, and the angle of incidence must be greater than the critical angle.

Cevap

Total internal reflection requires light to travel from an optically denser medium to an optically less dense medium with an angle of incidence greater than the critical angle.
For total internal reflection to happen, two strict conditions must be satisfied: (1) light must travel from a medium with a higher refractive index to one with a lower refractive index, and (2) the angle of incidence must be strictly greater than the critical angle for that boundary.

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1
Identify the optical density requirement
Light must attempt to pass from a medium of higher refractive index (denser) into a medium of lower refractive index (less dense) so that the refracted ray bends away from the normal.
Bending away from the normal allows the angle of refraction to reach 9090^\circ at the critical angle.
2
Identify the angle of incidence requirement
The angle of incidence in the denser medium must exceed the critical angle (i>Ci > C).
When the incidence angle exceeds the critical angle, no refraction is possible and all energy is reflected back into the denser medium.

Anahtar Kavram

Conditions for Total Internal Reflection
Soru 2Soru

The speed of light in medium AA is 1.5×108 m/s1.5 \times 10^8\text{ m/s} and in medium BB is 3.0×108 m/s3.0 \times 10^8\text{ m/s}. What is the critical angle for a light ray traveling from medium AA towards medium BB?

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Cevap: 3030^\circ

Cevap

The critical angle for light traveling from medium AA to medium BB is 3030^\circ.
The critical angle CC is the angle of incidence in the denser medium for which the angle of refraction in the rarer medium is 9090^\circ. Using the wave speed form of Snell's law, sinC=vAvB=1.5×1083.0×108=0.5\sin C = \frac{v_A}{v_B} = \frac{1.5 \times 10^8}{3.0 \times 10^8} = 0.5. Taking the inverse sine yields C=30C = 30^\circ.

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1
Determine the relationship between critical angle and wave speeds in the two media.
sinC=nBnA=vAvB\sin C = \frac{n_B}{n_A} = \frac{v_A}{v_B}
By Snell's Law, critical angle occurs when the angle of refraction is 9090^\circ, giving sinC=n2n1\sin C = \frac{n_2}{n_1}. Since refractive index n=cvn = \frac{c}{v}, the ratio nBnA\frac{n_B}{n_A} simplifies to vAvB\frac{v_A}{v_B}.
2
Substitute the given wave speeds into the equation.
sinC=1.5×108 m/s3.0×108 m/s=0.5\sin C = \frac{1.5 \times 10^8\text{ m/s}}{3.0 \times 10^8\text{ m/s}} = 0.5
Light is traveling from the optically denser medium AA (lower speed) to the less dense medium BB (higher speed).
3
Calculate the inverse sine to find the critical angle CC.
C=arcsin(0.5)=30C = \arcsin(0.5) = 30^\circ
The angle whose sine is 0.50.5 is 3030^\circ.

Anahtar Kavram

Critical Angle and Total Internal Reflection in terms of Wave Speed
Soru 3Soru

A water tank has a real depth of 16.0 cm16.0\text{ cm}. If the refractive index of water relative to air is 43\frac{4}{3}, what is the apparent depth of the tank in centimetres when viewed normally from above?

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Cevap: 12

Cevap

The apparent depth of the water tank is 12.0 cm12.0\text{ cm}.
When light passes from water to air, refraction causes the apparent depth to be smaller than the real depth by a factor equal to the refractive index nn. Substituting a real depth of 16.0 cm16.0\text{ cm} and n=43n = \frac{4}{3} into Apparent Depth=Real Depthn\text{Apparent Depth} = \frac{\text{Real Depth}}{n} yields 12.0 cm12.0\text{ cm}.

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1
Identify the relationship between refractive index, real depth, and apparent depth.
n=Real DepthApparent Depthn = \frac{\text{Real Depth}}{\text{Apparent Depth}}
Refraction at a plane boundary causes an object immersed in a denser medium to appear closer to the surface when viewed from a rarer medium.
2
Rearrange the equation to isolate Apparent Depth.
Apparent Depth=Real Depthn\text{Apparent Depth} = \frac{\text{Real Depth}}{n}
The unknown quantity requested by the question is the apparent depth.
3
Substitute the known numerical values into the equation.
Apparent Depth=16.043=16.0×34=12.0 cm\text{Apparent Depth} = \frac{16.0}{\frac{4}{3}} = 16.0 \times \frac{3}{4} = 12.0\text{ cm}
Dividing 16.016.0 by 43\frac{4}{3} gives 12.012.0.

Anahtar Kavram

Real and Apparent Depth in Light Refraction
Soru 4Soru

A light ray strikes the first face of a glass prism of refracting angle 3030^\circ at normal incidence (i=0i = 0^\circ). If the refractive index of the glass is 1.501.50, calculate the angle of emergence, in degrees, as the ray leaves the second face into air. (Take arcsin(0.75)=48.6\arcsin(0.75) = 48.6^\circ)

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Cevap: 48.6

Cevap

The angle of emergence of the light ray as it exits the prism is 48.648.6^\circ.
Because the ray is incident normally at the first surface, it continues undeviated into the glass (r1=0r_1 = 0^\circ). By prism geometry, the angle of incidence at the second face is equal to the apex angle of the prism (r2=A=30r_2 = A = 30^\circ). Applying Snell's Law at the glass-air boundary gives 1.50sin(30)=1.00sin(e)1.50 \sin(30^\circ) = 1.00 \sin(e), leading to sin(e)=0.75\sin(e) = 0.75, which evaluates to an emergent angle of 48.648.6^\circ.

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1
Determine the angle of refraction at the first surface
r1=0r_1 = 0^\circ
Light entering a surface normally (i1=0i_1 = 0^\circ) passes straight through without bending.
2
Find the angle of incidence at the second surface inside the prism using prism geometry
r2=30r_2 = 30^\circ
For any triangular prism, the refracting angle A=r1+r2A = r_1 + r_2. Since r1=0r_1 = 0^\circ, r2=A=30r_2 = A = 30^\circ.
3
Apply Snell's Law at the second interface (glass to air)
sin(e)=0.75\sin(e) = 0.75
nglasssin(r2)=nairsin(e)    1.50×sin(30)=1.00×sin(e)n_{\text{glass}} \sin(r_2) = n_{\text{air}} \sin(e) \implies 1.50 \times \sin(30^\circ) = 1.00 \times \sin(e).
4
Calculate the emergent angle ee
e=48.6e = 48.6^\circ
Taking the inverse sine of 0.750.75 yields e=arcsin(0.75)=48.6e = \arcsin(0.75) = 48.6^\circ.

Anahtar Kavram

Prism Geometry and Snell's Law Refraction
Soru 5Soru

A ray of light traveling inside a glass prism of refractive index 1.601.60 strikes the boundary with an adjacent oil medium of refractive index 1.201.20. What is the sine of the critical angle for total internal reflection at this glass-oil interface?

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Cevap: 0.750.75

Cevap

The sine of the critical angle at the glass-oil interface is 0.750.75.
For light traveling from a medium of refractive index n1n_1 into a medium of refractive index n2n_2 (where n1>n2n_1 > n_2), the critical angle CC satisfies sinC=n2n1\sin C = \frac{n_2}{n_1}. Substituting n1=1.60n_1 = 1.60 and n2=1.20n_2 = 1.20 gives sinC=1.201.60=0.75\sin C = \frac{1.20}{1.60} = 0.75.

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1
Identify the refractive indices of the two media.
Denser medium (glass): n1=1.60n_1 = 1.60; less dense medium (oil): n2=1.20n_2 = 1.20.
Total internal reflection occurs when light originates in the optically denser medium and strikes the boundary with a less dense medium.
2
Apply Snell's law at the critical angle CC.
n1sinC=n2sin90    sinC=n2n1n_1 \sin C = n_2 \sin 90^\circ \implies \sin C = \frac{n_2}{n_1}.
At the critical angle of incidence, the angle of refraction in the second medium is 9090^\circ, so sin90=1\sin 90^\circ = 1.
3
Substitute the given numerical values to compute sinC\sin C.
sinC=1.201.60=34=0.75\sin C = \frac{1.20}{1.60} = \frac{3}{4} = 0.75.
Dividing the refractive index of the oil by that of the glass gives the exact sine of the critical angle.

Anahtar Kavram

Critical Angle between Two Media
Soru 6Soru

A ray of light passes symmetrically through an equilateral glass prism of refractive index 2\sqrt{2}. What is the angle of minimum deviation of the ray, in degrees?

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Cevap: 30

Cevap

The angle of minimum deviation of the ray is 3030^\circ.
For an equilateral triangular prism, the apex angle AA is 6060^\circ. At minimum deviation, light travels symmetrically through the prism and obeys the exact relation n=sin(A+Dm2)sin(A2)n = \frac{\sin\left(\frac{A + D_m}{2}\right)}{\sin\left(\frac{A}{2}\right)}. Substituting n=2n = \sqrt{2} and A=60A = 60^\circ gives sin(60+Dm2)=22=sin(45)\sin\left(\frac{60^\circ + D_m}{2}\right) = \frac{\sqrt{2}}{2} = \sin(45^\circ). Equating arguments yields 60+Dm2=45\frac{60^\circ + D_m}{2} = 45^\circ, leading directly to Dm=30D_m = 30^\circ.

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1
Determine the refracting angle of the prism
A=60A = 60^\circ
An equilateral prism has interior angles of 6060^\circ each, so the apex angle A=60A = 60^\circ.
2
Set up the prism formula for minimum deviation
n=sin(A+Dm2)sin(A2)n = \frac{\sin\left(\frac{A + D_m}{2}\right)}{\sin\left(\frac{A}{2}\right)}
When light passes symmetrically through a prism, the deviation is at its minimum value DmD_m.
3
Substitute known values into the equation
2=sin(60+Dm2)sin(30)\sqrt{2} = \frac{\sin\left(\frac{60^\circ + D_m}{2}\right)}{\sin(30^\circ)}
Given n=2n = \sqrt{2} and A=60A = 60^\circ, with sin(30)=0.5\sin(30^\circ) = 0.5.
4
Calculate the sine of the half-angle
\sin\left(\frac{60^\circ + D_m}{2}\right) = \sqrt{2} \times 0.5 = \frac{\sqrt{2}}{2}
Multiplying both sides by sin(30)=0.5\sin(30^\circ) = 0.5.
5
Solve for the minimum deviation angle DmD_m
Dm=30D_m = 30^\circ
Since arcsin(22)=45\arcsin\left(\frac{\sqrt{2}}{2}\right) = 45^\circ, we set 60+Dm2=45    60+Dm=90    Dm=30\frac{60^\circ + D_m}{2} = 45^\circ \implies 60^\circ + D_m = 90^\circ \implies D_m = 30^\circ.

Anahtar Kavram

Refraction of light through a prism at the angle of minimum deviation
Soru 7Soru

A coin lies at the bottom of a vessel filled with a liquid to a depth of 14.0 cm14.0\text{ cm}. If the refractive index of the liquid relative to air is 1.401.40, calculate the apparent upward displacement of the coin in centimeters when viewed vertically from directly above.

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Cevap: 4

Cevap

The apparent upward displacement of the coin is 4.0 cm4.0\text{ cm}.
Refraction at the liquid-air boundary makes an object at real depth h=14.0 cmh = 14.0\text{ cm} appear at an apparent depth h=hn=14.01.40=10.0 cmh' = \frac{h}{n} = \frac{14.0}{1.40} = 10.0\text{ cm}. The apparent upward displacement is the difference between real depth and apparent depth: d=14.0 cm10.0 cm=4.0 cmd = 14.0\text{ cm} - 10.0\text{ cm} = 4.0\text{ cm}.

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1
Identify the given values and formula for refractive index in terms of depth.
Real depth h=14.0 cmh = 14.0\text{ cm}, refractive index n=1.40n = 1.40. Formula: n=Real depthApparent depth=hhn = \frac{\text{Real depth}}{\text{Apparent depth}} = \frac{h}{h'}.
Light rays bending away from the normal upon leaving the denser liquid cause the coin to appear closer to the surface.
2
Calculate the apparent depth (hh').
h=14.0 cm1.40=10.0 cmh' = \frac{14.0\text{ cm}}{1.40} = 10.0\text{ cm}.
Rearranging the refractive index formula gives h=hnh' = \frac{h}{n}.
3
Calculate the apparent upward displacement (dd).
d=hh=14.0 cm10.0 cm=4.0 cmd = h - h' = 14.0\text{ cm} - 10.0\text{ cm} = 4.0\text{ cm}.
The displacement is the distance between the actual position at the bottom and the virtual image position.

Anahtar Kavram

Real depth, apparent depth, and apparent displacement
Soru 8Soru

A ray of light traveling in air strikes the flat surface of a transparent glass slab at an angle of incidence of 6060^\circ. If the refractive index of the glass slab relative to air is 3\sqrt{3}, what is the angle of refraction inside the glass slab in degrees?

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Cevap: 30

Cevap

The angle of refraction inside the glass slab is 3030^\circ.
According to Snell's Law, n=sinisinrn = \frac{\sin i}{\sin r}. Substituting n=3n = \sqrt{3} and i=60i = 60^\circ gives 3=sin60sinr\sqrt{3} = \frac{\sin 60^\circ}{\sin r}. Since sin60=32\sin 60^\circ = \frac{\sqrt{3}}{2}, rearranging gives sinr=3/23=0.5\sin r = \frac{\sqrt{3}/2}{\sqrt{3}} = 0.5. Taking the inverse sine of 0.50.5 gives r=30r = 30^\circ.

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1
Identify Snell's law formula relating the angle of incidence and angle of refraction.
n=sinisinrn = \frac{\sin i}{\sin r}
Snell's law describes how light bends when crossing the boundary between two optical media.
2
Substitute the given values i=60i = 60^\circ and n=3n = \sqrt{3} into the equation.
3=sin60sinr\sqrt{3} = \frac{\sin 60^\circ}{\sin r}
Plugging in the known parameters allows us to isolate the unknown sine of the angle of refraction.
3
Substitute sin60=32\sin 60^\circ = \frac{\sqrt{3}}{2} and rearrange for sinr\sin r.
\sin r = \frac{\sqrt{3}/2}{\sqrt{3}} = 0.5
Canceling 3\sqrt{3} from both sides yields a simple numerical value for sinr\sin r.
4
Take the inverse sine of 0.50.5 to find rr.
r=arcsin(0.5)=30r = \arcsin(0.5) = 30^\circ
The angle whose sine is 0.50.5 is 3030^\circ.

Anahtar Kavram

Snell's Law of Refraction
Soru 9Soru

A rectangular glass block of thickness 6.0 cm6.0\text{ cm} has a refractive index of 1.501.50. Calculate the apparent depth, in centimeters, of a mark placed at the bottom of the block when viewed normally from above.

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Cevap: 4

Cevap

The apparent depth of the mark is 4.0 cm4.0\text{ cm}.
The refractive index of a medium relative to air is given by the ratio of real depth to apparent depth (n=Real DepthApparent Depthn = \frac{\text{Real Depth}}{\text{Apparent Depth}}). Substituting the given values gives Apparent Depth=6.0 cm1.50=4.0 cm\text{Apparent Depth} = \frac{6.0\text{ cm}}{1.50} = 4.0\text{ cm}.

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1
Identify the relationship between refractive index, real depth, and apparent depth for normal view
n=Real DepthApparent Depthn = \frac{\text{Real Depth}}{\text{Apparent Depth}}
By definition of optical refraction when looking normally from an optically less dense medium (air) into a denser medium (glass).
2
Substitute the known values (n=1.50n = 1.50, Real Depth=6.0 cm\text{Real Depth} = 6.0\text{ cm}) and solve for the apparent depth
\text{Apparent Depth} = \frac{6.0\text{ cm}}{1.50} = 4.0\text{ cm}
Dividing the real thickness by the refractive index yields the perceived (apparent) depth.

Anahtar Kavram

Real and Apparent Depth in Refraction
Soru 10Soru

Which of the following conditions must be satisfied for light to undergo total internal reflection at the boundary between two transparent media?

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Cevap: The light ray must travel from an optically denser medium into an optically less dense medium, and the angle of incidence must exceed the critical angle.

Cevap

The light ray must travel from an optically denser medium into an optically less dense medium, and the angle of incidence must exceed the critical angle.
Total internal reflection occurs only when light passes from a medium of higher optical density into a medium of lower optical density, and the angle of incidence exceeds the critical angle for that boundary.

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1
Identify the boundary requirement for wave propagation direction in total internal reflection.
Light must travel from an optically denser medium (higher refractive index n1n_1) toward an optically rarer medium (lower refractive index n2n_2).
This direction allows the ray to bend away from the normal, increasing the angle of refraction relative to the angle of incidence.
2
Determine the required angle of incidence at the boundary.
The angle of incidence ii must be strictly greater than the critical angle θc\theta_c (where sinθc=n2/n1\sin \theta_c = n_2 / n_1).
When i>θci > \theta_c, no refraction can take place because sinr>1\sin r > 1, forcing all light energy to reflect back into the initial denser medium.

Anahtar Kavram

Conditions for Total Internal Reflection
Soru 11Soru

A swimming pool has an apparent depth of 1.8 m1.8\text{ m} when viewed vertically from directly above. If the refractive index of water relative to air is 43\frac{4}{3}, what is the real depth of the pool in meters?

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Cevap: 2.4

Cevap

The real depth of the pool is 2.4 m2.4\text{ m}.
The refractive index nn of a medium is defined as the ratio of the real depth to the apparent depth (n=Real DepthApparent Depthn = \frac{\text{Real Depth}}{\text{Apparent Depth}}). Multiplying the observed apparent depth of 1.8 m1.8\text{ m} by the refractive index 43\frac{4}{3} gives the true real depth of 2.4 m2.4\text{ m}.

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1
Identify the relationship between refractive index, real depth, and apparent depth.
Refractive index n=Real DepthApparent Depthn = \frac{\text{Real Depth}}{\text{Apparent Depth}}.
Light bending at the boundary causes an object submerged in a denser medium to appear closer to the surface.
2
Rearrange the equation to make Real Depth the subject.
\text{Real Depth} = n \times \text{Apparent Depth}.
To calculate the true depth from the observed apparent depth and the optical density of water.
3
Substitute the given values into the formula.
\text{Real Depth} = \frac{4}{3} \times 1.8\text{ m} = 2.4\text{ m}.
Multiplying the apparent depth by the refractive index yields the actual physical depth.

Anahtar Kavram

Refraction of Light and Real/Apparent Depth
Soru 12Soru

A small object lies at the bottom of a transparent vessel containing two immiscible liquid layers, AA and BB. Layer AA (top) has a real thickness of 7.0 cm7.0\text{ cm} and a refractive index of 1.401.40. Layer BB (bottom) has a real thickness of 8.0 cm8.0\text{ cm} and a refractive index of 1.601.60. Calculate the apparent displacement of the object, in centimeters, when viewed vertically from directly above.

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Cevap: 5

Cevap

The apparent displacement of the object is 5.0 cm5.0\text{ cm}.
For multiple refractive layers viewed normally, the total apparent depth is the sum of individual layer apparent depths: 7.01.40+8.01.60=5.0+5.0=10.0 cm\frac{7.0}{1.40} + \frac{8.0}{1.60} = 5.0 + 5.0 = 10.0\text{ cm}. Subtracting this total apparent depth from the total real depth of 15.0 cm15.0\text{ cm} gives an apparent vertical shift (displacement) of 5.0 cm5.0\text{ cm}.

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1
Calculate the apparent depth of the top liquid layer (Layer A)
Apparent depth of Layer A = 5.0 cm5.0\text{ cm}
Apparent depth for a single medium is obtained by dividing real depth by its refractive index: 7.01.40=5.0 cm\frac{7.0}{1.40} = 5.0\text{ cm}.
2
Calculate the apparent depth of the bottom liquid layer (Layer B)
Apparent depth of Layer B = 5.0 cm5.0\text{ cm}
Apparent depth for Layer B is 8.01.60=5.0 cm\frac{8.0}{1.60} = 5.0\text{ cm}.
3
Calculate total real depth and total apparent depth
Total real depth = 15.0 cm15.0\text{ cm}; Total apparent depth = 10.0 cm10.0\text{ cm}
Depths in composite media are additive.
4
Calculate vertical apparent displacement
Apparent displacement = 5.0 cm5.0\text{ cm}
Displacement is the difference between total real depth and total apparent depth: 15.0 cm10.0 cm=5.0 cm15.0\text{ cm} - 10.0\text{ cm} = 5.0\text{ cm}.

Anahtar Kavram

Refraction through composite media and vertical apparent displacement
Soru 13Soru

A light ray traveling inside a transparent glass prism of refractive index 1.501.50 strikes the boundary with air. What is the sine of the critical angle (sinC\sin C) for total internal reflection to occur at this boundary?

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Cevap: 0.670.67

Cevap

The sine of the critical angle (sinC\sin C) for total internal reflection at the glass-air boundary is 0.670.67.
For light moving from a medium with refractive index nn into air, total internal reflection occurs when the angle of incidence exceeds the critical angle CC. The critical angle satisfies sinC=1n\sin C = \frac{1}{n}. Substituting n=1.50n = 1.50 gives sinC=11.50=0.67\sin C = \frac{1}{1.50} = 0.67.

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1
Identify the relationship between the refractive index (nn) and the critical angle (CC) when light travels from a medium to air.
sinC=1n\sin C = \frac{1}{n}
By Snell's law, at the critical angle of incidence, the angle of refraction in air is 9090^\circ (so sin90=1\sin 90^\circ = 1).
2
Substitute the given refractive index (n=1.50n = 1.50) into the formula.
sinC=11.50=230.67\sin C = \frac{1}{1.50} = \frac{2}{3} \approx 0.67
Dividing 11 by 1.501.50 yields 0.666...0.666..., which rounds to 0.670.67.

Anahtar Kavram

Critical Angle and Total Internal Reflection
Tahmini Süre:45s
Soru 14Soru

A light ray enters the first face of a glass prism surrounded by air. The prism has a refracting angle of 7575^\circ and a refractive index of 2\sqrt{2}. Inside the prism, the ray strikes the second refracting face at the critical angle for total internal reflection. Calculate the angle of incidence, in degrees, at the first face.

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Cevap: 45

Cevap

The angle of incidence at the first face is 4545^\circ.
To find the angle of incidence at the first face, first determine the critical angle CC at the second glass-air surface using sinC=1n=12\sin C = \frac{1}{n} = \frac{1}{\sqrt{2}}, which yields C=45C = 45^\circ. Since the ray strikes the second face at this critical angle, r2=45r_2 = 45^\circ. Next, using the geometric relationship for a prism A=r1+r2A = r_1 + r_2, the angle of refraction at the first surface is r1=Ar2=7545=30r_1 = A - r_2 = 75^\circ - 45^\circ = 30^\circ. Finally, applying Snell's law at the first face gives sini=nsinr1=2sin30=22\sin i = n \sin r_1 = \sqrt{2} \sin 30^\circ = \frac{\sqrt{2}}{2}. Taking the inverse sine yields i=45i = 45^\circ.

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1
Find the critical angle at the second face
Critical angle C=45C = 45^\circ, so r2=45r_2 = 45^\circ
Light travels from glass to air at the critical angle, so sinC=1n=12\sin C = \frac{1}{n} = \frac{1}{\sqrt{2}}.
2
Determine the angle of refraction at the first face
r1=30r_1 = 30^\circ
The apex angle of a prism satisfies A=r1+r2A = r_1 + r_2, hence r1=Ar2=7545=30r_1 = A - r_2 = 75^\circ - 45^\circ = 30^\circ.
3
Apply Snell's Law at the entry boundary
sini=22\sin i = \frac{\sqrt{2}}{2}
Refraction at the first surface gives sini=nsinr1=2sin30=2×0.5=22\sin i = n \sin r_1 = \sqrt{2} \sin 30^\circ = \sqrt{2} \times 0.5 = \frac{\sqrt{2}}{2}.
4
Solve for the incident angle ii
i=45i = 45^\circ
arcsin(22)=45\arcsin\left(\frac{\sqrt{2}}{2}\right) = 45^\circ.

Anahtar Kavram

Refraction through a prism combined with total internal reflection critical angle condition
Soru 15Soru

A light wave travels through medium A at a speed of 2.25×108 m s12.25 \times 10^8\text{ m s}^{-1} and enters medium B, where its speed decreases to 1.50×108 m s11.50 \times 10^8\text{ m s}^{-1}. What is the value of the sine of the critical angle for total internal reflection between these two media, and in which medium must the light ray originate?

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Cevap: 23\frac{2}{3}, originating in medium B

Cevap

The sine of the critical angle is 23\frac{2}{3}, and the light ray must originate in medium B.
Total internal reflection occurs when light travels from an optically denser medium to an optically rarer medium. Since the speed of light is lower in medium B (1.50×108 m s11.50 \times 10^8\text{ m s}^{-1}) than in medium A (2.25×108 m s12.25 \times 10^8\text{ m s}^{-1}), medium B is the denser medium. The critical angle CC satisfies sinC=vdensevrare=1.50×1082.25×108=23\sin C = \frac{v_{\text{dense}}}{v_{\text{rare}}} = \frac{1.50 \times 10^8}{2.25 \times 10^8} = \frac{2}{3}. Therefore, the light must originate in medium B and the sine of the critical angle is 23\frac{2}{3}.

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1
Determine the relative optical densities of medium A and medium B from wave speed
Medium B has a lower light speed (1.50×108 m s11.50 \times 10^8\text{ m s}^{-1}) than medium A (2.25×108 m s12.25 \times 10^8\text{ m s}^{-1}), so medium B is optically denser than medium A.
Refractive index is inversely proportional to wave speed (n1vn \propto \frac{1}{v}).
2
Identify the required direction of light propagation for total internal reflection
The light ray must originate in medium B and travel toward medium A.
Total internal reflection occurs only when light attempts to pass from a medium of higher refractive index (denser) to a medium of lower refractive index (rarer).
3
Calculate the sine of the critical angle
sinC=vBvA=1.50×1082.25×108=23\sin C = \frac{v_B}{v_A} = \frac{1.50 \times 10^8}{2.25 \times 10^8} = \frac{2}{3}.
By Snell's law at the critical angle, sinC=nAnB=vBvA\sin C = \frac{n_A}{n_B} = \frac{v_B}{v_A}.

Anahtar Kavram

Conditions for Total Internal Reflection and Critical Angle calculation from wave speeds
Tahmini Süre:1m 30s
Soru 16Soru

A glass prism with a refracting angle of 6060^\circ has a refractive index of 2\sqrt{2}. What is the angle of minimum deviation, in degrees, experienced by a light ray passing through this prism?

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Cevap: 30

Cevap

The angle of minimum deviation is 3030^\circ.
Using the prism minimum deviation relation n=sin((A+Dm)/2)sin(A/2)n = \frac{\sin\left((A + D_m)/2\right)}{\sin(A/2)}, substituting n=2n = \sqrt{2} and A=60A = 60^\circ yields sin((60+Dm)/2)=12\sin\left((60^\circ + D_m)/2\right) = \frac{1}{\sqrt{2}}. This gives (60+Dm)/2=45(60^\circ + D_m)/2 = 45^\circ, so Dm=30D_m = 30^\circ.

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1
Apply the prism minimum deviation equation.
n=sin(A+Dm2)sin(A2)n = \frac{\sin\left(\frac{A + D_m}{2}\right)}{\sin\left(\frac{A}{2}\right)}
This relates refractive index, prism refracting angle, and minimum deviation angle.
2
Substitute the given values A=60A = 60^\circ and n=2n = \sqrt{2}.
2=sin(60+Dm2)sin(30)\sqrt{2} = \frac{\sin\left(\frac{60^\circ + D_m}{2}\right)}{\sin(30^\circ)}
Dividing the refracting angle 6060^\circ by 2 gives 3030^\circ for the denominator angle.
3
Calculate the numerator sine term.
sin(60+Dm2)=12\sin\left(\frac{60^\circ + D_m}{2}\right) = \frac{1}{\sqrt{2}}
Multiplying 2\sqrt{2} by sin(30)=0.5\sin(30^\circ) = 0.5 gives 22=12\frac{\sqrt{2}}{2} = \frac{1}{\sqrt{2}}.
4
Solve for the angle DmD_m.
Dm=30D_m = 30^\circ
Since arcsin(12)=45\arcsin\left(\frac{1}{\sqrt{2}}\right) = 45^\circ, we have 60+Dm2=45\frac{60^\circ + D_m}{2} = 45^\circ, leading to 60+Dm=9060^\circ + D_m = 90^\circ.

Anahtar Kavram

Minimum Deviation in Triangular Prisms
Soru 17Soru

A block of transparent polymer with a refractive index of 1.251.25 is placed over a small mark on a table. When viewed vertically from directly above, the mark appears to be shifted upward by 3.0 cm3.0\text{ cm}. What is the real thickness of the polymer block in centimeters?

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Cevap: 15

Cevap

The real thickness of the polymer block is 15.0 cm15.0\text{ cm}.
Refraction at the interface produces an upward shift s=d(11n)s = d\left(1 - \frac{1}{n}\right). Substituting s=3.0 cms = 3.0\text{ cm} and n=1.25n = 1.25 gives 3.0=d(10.80)=0.20d3.0 = d(1 - 0.80) = 0.20d, which solves to a real thickness d=15.0 cmd = 15.0\text{ cm}.

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1
Relate apparent depth dd' to real depth dd using the refractive index.
d=dnd' = \frac{d}{n}
Light refracting at the surface of a denser medium causes the object to appear at a shallower depth.
2
Express the apparent displacement (upward shift) ss in terms of dd and nn.
s=dd=d(11n)s = d - d' = d\left(1 - \frac{1}{n}\right)
The upward shift is the vertical distance between the true position and the apparent position.
3
Substitute s=3.0 cms = 3.0\text{ cm} and n=1.25n = 1.25 into the equation and solve for dd.
3.0=d(111.25)=d(10.80)=0.20d    d=15.0 cm3.0 = d\left(1 - \frac{1}{1.25}\right) = d(1 - 0.80) = 0.20 d \implies d = 15.0\text{ cm}
Algebraic evaluation yields the exact real thickness of the polymer block.

Anahtar Kavram

Apparent depth and upward displacement due to refraction
Soru 18Soru

An optical fiber consists of a core with a refractive index of 1.501.50 surrounded by a cladding with a refractive index of 1.201.20. Which of the following correctly describes the direction a light ray must travel for total internal reflection to take place at the boundary, as well as the sine of the critical angle?

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Cevap: From core to cladding with sinC=0.80\sin C = 0.80

Cevap

Light must travel from the core to the cladding with sinC=0.80\sin C = 0.80
Total internal reflection takes place only when light travels from an optically denser medium (n1=1.50n_1 = 1.50) to an optically less dense medium (n2=1.20n_2 = 1.20). Applying Snell's law at the critical boundary gives sinC=n2n1=1.201.50=0.80\sin C = \frac{n_2}{n_1} = \frac{1.20}{1.50} = 0.80.

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1
Determine the direction requirement for Total Internal Reflection (TIR)
Light must travel from the denser medium (core, n1=1.50n_1 = 1.50) toward the less dense medium (cladding, n2=1.20n_2 = 1.20).
TIR only occurs when light attempts to pass into a medium of lower optical density so that the refracted ray bends away from the normal.
2
Calculate the sine of the critical angle CC
\sin C = \frac{n_2}{n_1} = \frac{1.20}{1.50} = 0.80
By Snell's law at the critical angle, n1sinC=n2sin90    sinC=n2n1n_1 \sin C = n_2 \sin 90^\circ \implies \sin C = \frac{n_2}{n_1}.

Anahtar Kavram

Total Internal Reflection and Critical Angle
Tahmini Süre:1m 30s
Soru 19Soru

A beam of monochromatic light travels through a transparent liquid toward a boundary with air. The speed of light in the liquid is 1.80×108 m s11.80 \times 10^8\text{ m s}^{-1} and the speed of light in air is 3.00×108 m s13.00 \times 10^8\text{ m s}^{-1}. What is the value of the sine of the critical angle (sinC\sin C) for total internal reflection at this boundary, and under what condition of propagation can total internal reflection occur?

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Cevap: sinC=0.60\sin C = 0.60, and the light ray must travel from the liquid into air.

Cevap

The sine of the critical angle is sinC=0.60\sin C = 0.60, and total internal reflection can only occur when light travels from the optically denser liquid into air.
Total internal reflection requires light to originate in the optically denser medium (the liquid) and travel toward the rarer medium (air), at an angle of incidence greater than the critical angle. The sine of the critical angle is calculated directly as the ratio of the speed of light in the medium to the speed of light in air: sinC=vliquidvair=1.80×1083.00×108=0.60\sin C = \frac{v_{\text{liquid}}}{v_{\text{air}}} = \frac{1.80 \times 10^8}{3.00 \times 10^8} = 0.60.

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1
Determine the refractive index nn of the liquid relative to air.
n=cv=3.00×108 m s11.80×108 m s1=1.67n = \frac{c}{v} = \frac{3.00 \times 10^8\text{ m s}^{-1}}{1.80 \times 10^8\text{ m s}^{-1}} = 1.67 (or 53\frac{5}{3}).
Refractive index is the ratio of the speed of light in vacuum/air to the speed of light in the medium.
2
Calculate the sine of the critical angle sinC\sin C.
sinC=1n=vc=1.80×1083.00×108=0.60\sin C = \frac{1}{n} = \frac{v}{c} = \frac{1.80 \times 10^8}{3.00 \times 10^8} = 0.60.
The critical angle relationship between a medium and air is given by sinC=1n\sin C = \frac{1}{n}.
3
Identify the necessary physical condition for total internal reflection to take place.
Light must travel from an optically denser medium (liquid) toward an optically less dense medium (air).
For total internal reflection to happen, the ray must bend away from the normal until the angle of refraction reaches 9090^\circ. This only occurs when moving from a denser to a rarer medium.

Anahtar Kavram

Critical Angle and Conditions for Total Internal Reflection
Tahmini Süre:1m 15s
Soru 20Soru

A container holds a layer of water of depth 16.0 cm16.0\text{ cm}. An immiscible layer of oil of refractive index 1.201.20 and thickness 6.0 cm6.0\text{ cm} floats on top of the water. If the refractive index of water is 1.331.33 (or 43\frac{4}{3}), what is the total apparent depth, in centimeters, of a small object resting at the bottom of the container when viewed normally from directly above?

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Cevap: 17

Cevap

The total apparent depth of the object when viewed normally from directly above is 17.0 cm17.0\text{ cm}.
When an object at the bottom of a container is viewed normally through multiple transparent media, the overall apparent depth is the sum of the apparent depths produced by each medium individually (dapp=dinid_{\text{app}} = \sum \frac{d_i}{n_i}). Substituting the given values gives 16.04/3+6.01.20=12.0 cm+5.0 cm=17.0 cm\frac{16.0}{4/3} + \frac{6.0}{1.20} = 12.0\text{ cm} + 5.0\text{ cm} = 17.0\text{ cm}.

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1
Calculate the apparent depth of the water layer.
Apparent depth of water = 12.0 cm12.0\text{ cm}
Apparent depth in a single medium is given by the real depth divided by its refractive index (dapp=d/nd_{\text{app}} = d / n). For water, 16.04/3=12.0 cm\frac{16.0}{4/3} = 12.0\text{ cm}.
2
Calculate the apparent depth of the oil layer.
Apparent depth of oil = 5.0 cm5.0\text{ cm}
Using dapp=d/nd_{\text{app}} = d / n for the oil layer, 6.01.20=5.0 cm\frac{6.0}{1.20} = 5.0\text{ cm}.
3
Sum the apparent depths of both media.
Total apparent depth = 17.0 cm17.0\text{ cm}
For multiple parallel transparent layers, the total apparent depth is the sum of the apparent depths of each individual layer.

Anahtar Kavram

Apparent depth in composite media layers
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Refraction of Light, Total Internal Reflection, and Prisms Alıştırma Soruları — JAMB UTME | Examkin