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Original question & working

A reflected laser and a sensor-distance check · source reference

[2017/YJC/Prelim/I/12] · Question pp. 7 · Working pp. 34, 35, 36

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The working and teaching notes are included in the interactive lesson.

For beam distances, check the foot lies on the actual ray or incident segment; an infinite-line distance alone may be insufficient.

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Full original question, working & notes

Printed question

Laser (Light Amplification by Stimulated Emission of Radiation) has many applications including medicine, data storage, military and industrial uses. It has the property of spatial coherence, which allows the laser beam to stay narrow over long distances. When a laser beam is projected onto a mirror at an angle, it reflects off the mirror at the same angle.

An engineer is designing a device that does industrial cutting using a laser beam. To make the device compact, the device has a mirror to reflect the beam before it leaves the device. The laser beam source is located at the origin OO. It projects an incident beam with direction vector i+2j+k\mathbf i+2\mathbf j+\mathbf k. The beam hits the mirror at the point PP with angle θ\theta. The mirror has an equation −x+2y+3z=12-x+2y+3z=12.

Native source reflection diagram

(i) Find the acute angle θ\theta that the beam makes with the mirror. [2]

(ii) By finding O′O', the image of OO in the mirror, find a vector equation of the line that the reflected beam is on. [7]

The engineer plans to install a sensor at (3,1,0)(3,1,0) to monitor the heat produced by the laser. For the sensor to work properly, the sensor must be less than 2 units away from either the incident or the reflected beam. Determine if the sensor will work properly. [4]

[2017/YJC/Prelim/I/12]

Printed working

(i) Let α=90∘−θ\alpha=90^\circ-\theta. (Note that α\alpha is also an acute angle).

Then cos⁡α=∣(−1,2,3)⋅(1,2,1)∣∣(−1,2,3)∣∣(1,2,1)∣=∣−1+4+3∣1+4+91+4+1=66(14)\cos\alpha=\frac{|(-1,2,3)\cdot(1,2,1)|}{|(-1,2,3)||(1,2,1)|}=\frac{|-1+4+3|}{\sqrt{1+4+9}\sqrt{1+4+1}}=\frac6{\sqrt{6(14)}}.

⇒α=49.1066∘\Rightarrow\alpha=49.1066^\circ.

Thus, θ=90∘−49.1066∘=40.9∘\theta=90^\circ-49.1066^\circ=40.9^\circ (correct to 1 d.p.).

(ii) Let NN be the foot of perpendicular from OO to mirror plane.

Then ON→=λ(−1,2,3)\overrightarrow{ON}=\lambda(-1,2,3) for some λ∈R\lambda\in\mathbb R.

Since NN lies on the plane, ON→⋅(−1,2,3)=12\overrightarrow{ON}\cdot(-1,2,3)=12.

Thus λ(−1,2,3)⋅(−1,2,3)=12⇒λ(1+4+9)=12⇒λ=1214=67\lambda(-1,2,3)\cdot(-1,2,3)=12\Rightarrow\lambda(1+4+9)=12\Rightarrow\lambda=\frac{12}{14}=\frac67.

Therefore, ON→=67(−1,2,3)\overrightarrow{ON}=\frac67(-1,2,3).

Since O′O' is the reflection of OO in the plane, OO′→=2ON→=127(−1,2,3)\overrightarrow{OO'}=2\overrightarrow{ON}=\frac{12}7(-1,2,3).

OP→=μ(1,2,1)\overrightarrow{OP}=\mu(1,2,1) for some μ∈R\mu\in\mathbb R.

Since PP lies on the plane, OP→⋅(−1,2,3)=12\overrightarrow{OP}\cdot(-1,2,3)=12.

Thus μ(1,2,1)⋅(−1,2,3)=12⇒μ(−1+4+3)=12⇒μ=2\mu(1,2,1)\cdot(-1,2,3)=12\Rightarrow\mu(-1+4+3)=12\Rightarrow\mu=2.

Therefore, OP→=2(1,2,1)=(2,4,2)\overrightarrow{OP}=2(1,2,1)=(2,4,2).

A direction vector of reflected beam is O′P→\overrightarrow{O'P}

=(2,4,2)−127(−1,2,3)=17(14+12,28−24,14−36)=17(26,4,−22)=27(13,2,−11)=(2,4,2)-\frac{12}7(-1,2,3)=\frac17(14+12,28-24,14-36)=\frac17(26,4,-22)=\frac27(13,2,-11).

Thus equation of reflected beam is r=(2,4,2)+δ(13,2,−11)\mathbf r=(2,4,2)+\delta(13,2,-11), δ∈R\delta\in\mathbb R.

Sensor distances

Let BB be the point (3,1,0)(3,1,0).

Shortest distance of BB from incident beam

=∣(3,1,0)×(1,2,1)∣1+4+1=∣(1,−3,5)∣6=356>2=\frac{|(3,1,0)\times(1,2,1)|}{\sqrt{1+4+1}}=\frac{|(1,-3,5)|}{\sqrt6}=\sqrt{\frac{35}6}>2.

Shortest distance of BB from reflected beam

=∣(1,−3,−2)×(13,2,−11)∣169+4+121=∣(37,−15,41)∣294=3275294>2=\frac{|(1,-3,-2)\times(13,2,-11)|}{\sqrt{169+4+121}}=\frac{|(37,-15,41)|}{\sqrt{294}}=\sqrt{\frac{3275}{294}}>2.

Since the shortest distance from BB to both beams are greater than 2, the sensor will not work.

Native source teaching diagram, Q20 angle Native source teaching diagram, Q20 reflection Native source teaching diagram, Q20 incident-distance Native source teaching diagram, Q20 reflected-distance

Printed answer key

(i) 40.9∘40.9^\circ. (ii) OO′→=127(−1,2,3)\overrightarrow{OO'}=\frac{12}7(-1,2,3); r=(2,4,2)+δ(13,2,−11)\mathbf r=(2,4,2)+\delta(13,2,-11), δ∈R\delta\in\mathbb R. Short key omits the sensor verdict.

Editorial qualification

The printed vector equation uses a full supporting line with parameter in R\mathbb R. The physical reflected beam is the outgoing ray r=(2,4,2)+t(13,2,−11)r=(2,4,2)+t(13,2,-11), t≥0t\ge0. For the sensor S=(3,1,0)S=(3,1,0), (S−P)⋅(13,2,−11)=29(S-P)\cdot(13,2,-11)=29, so the reflected perpendicular foot has parameter t=29/294>0t=29/294>0 and lies on the actual ray. The incident foot has parameter 5/65/6, within the segment from OO to PP (parameters 0≤t≤20\le t\le2). Thus both supporting-line distances apply to the actual beams: 35/6\sqrt{35/6} and 3275/294\sqrt{3275/294}, both greater than 2. The sensor will not work. This corrects an earlier native editorial claim that the reflected parameter was negative; the printed source working is retained.

Source provenance

2025 TJC H2 Math (9758) JC2 MSM: VECTORS. Question booklet PDF pages 4–12 (printed 80–88); solution booklet PDF pages 17–44. Column vectors are typeset as ordered coordinate triples here; the entries, products, intermediate equations and original parameter/domain restrictions are retained.