Animated Solution for Mathematics - Straight Lines: A ray of light coming from the point (2,23) is incident at an angle 30∘ on the line x=1 at the point A. The ray gets reflected on the line x=1 and meets x-axis at the point B. Then, the line AB passes through the point:
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Visualized Solution
Setting up the Coordinate System
Given point P(2,23)
Mirror line: x=1
The Incident Ray and Angle
A ray from P strikes the mirror at point A.
Angle with the mirror line x=1 is 30∘.
Slope of the Incident Ray
Angle with the normal =90∘−30∘=60∘
Slope of incident ray PA=tan(60∘)=3
Setting up Coordinates for Point A
Point A lies on x=1, so A=(1,yA)
Slope formula: m=x2−x1y2−y1
Calculating the Coordinates of A
2−123−yA=3
23−yA=3⟹yA=3
Point A=(1,3)
The Reflection Principle
The reflected ray appears to originate from the virtual image of P.
Let the image of P across x=1 be P′.
Coordinates of Image Point P′
Distance of P(2,23) from x=1 is 1 unit.
P′ is 1 unit to the left of x=1.
P′=(0,23)
Tracing the Reflected Ray
The reflected ray passes through A and P′.
It travels from A towards the x-axis, meeting it at B.
Slope of the Reflected Ray
Line passes through P′(0,23) and A(1,3).
Slope m′=1−03−23
Calculating the Slope m′
m′=1−3=−3
Equation of the Reflected Ray
Using point-slope form with P′(0,23):
y−23=−3(x−0)
y=−3x+23
Checking the Given Options
We need to find which option lies on y=−3x+23.
Let's test the point (3,−3).
Final Confirmation
Substitute x=3 into the equation:
y=−3(3)+23
y=−33+23=−3
The point (3,−3) satisfies the equation!
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The Sigma Insight: Various Forms of Equations of a Line
Solution Diagram
The Dance of Light
A Journey Through Reflection
Imagine you are standing in a dark room, holding a laser pointer. You aim it at a mirror, watching the beam dance across the wall. In the world of JEE Advanced, this isn't just a light show; it is a beautiful interplay of geometry and algebra.
Today, we are going to master the reflection of a ray of light off a vertical mirror, turning a seemingly complex path into a simple, elegant line equation.
Phase 1
The Incident Ray
We begin with a source point P(2,23) and a mirror defined by the line x=1. The ray strikes the mirror at point A.
The problem states the ray makes an angle of 30∘ with the mirror. Since our mirror is the vertical line x=1, the normal is a horizontal line. Thus, the angle the ray makes with the normal is 90∘−30∘=60∘.
To find the slope of the incident ray PA, we use the tangent of the angle it makes with the horizontal: m=tan(60∘)=3. Since the ray passes through P(2,23) and A lies on x=1, we use the slope formula:
2−123−yA=3
Solving this, we find 23−yA=3, which gives us yA=3. So, our point of incidence is A(1,3).
Phase 2
The Virtual Image Shortcut
We could use the law of reflection to find the angle of the reflected ray, but there is a more elegant way. In physics, we know that a reflected ray appears to originate from the virtual image of the source point.
Let P′ be the reflection of P(2,23) across the line x=1. Since P is 1 unit to the right of the mirror, P′ must be 1 unit to the left. Thus, P′=(0,23).
This is the 'Aha!' moment. The reflected ray is simply the straight line connecting the virtual image P′ and the point of incidence A. We have effectively turned a reflection problem into a simple line-through-two-points problem.
Phase 3
The Final Equation
We now have two points on our reflected ray: P′(0,23) and A(1,3). The slope m′ of this line is:
m′=1−03−23=−3
Using the point-slope form y−y1=m(x−x1) with point P′, we get:
y−23=−3(x−0)
This simplifies beautifully to the final equation of the reflected ray:
y=−3x+23
Phase 4
The Victory Lap
We are looking for a point that lies on this line. We test the provided coordinate (3,−3):
y=−3(3)+23=−33+23=−3
It matches perfectly! The point (3,−3) lies exactly on the path of the reflected ray.
You have successfully navigated the geometry, utilized the power of virtual images, and arrived at the solution with mathematical precision. Remember, in physics, every complex path is just a collection of simple, logical steps.