Animated Solution for Mathematics - Straight Lines: A ray of light along x+3y=3 gets reflected upon reaching x-axis, the equation of the reflected ray is
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Visualized Solution
Visualizing the Setup
Incident ray equation: x+3y=3
Reflecting surface: x-axis (y=0)
Finding the Point of Incidence
The ray hits the x-axis.
At the x-axis, the y-coordinate is always 0.
Substituting y=0
Substitute y=0 into the incident ray equation:
x+3(0)=3
Point of Incidence A
x=3
Point of incidence: A(3,0)
The Image Point Method
A reflected ray appears to originate from the virtual image of the incident ray.
We need one more point on the incident ray to find its image.
Finding Point B on Incident Ray
Let's find the y-intercept by setting x=0.
0+3y=3
Coordinates of Point B
3y=3⟹y=1
Point on incident ray: B(0,1)
Reflecting Point B
The mirror is the x-axis (y=0).
Reflection of (x,y) across the x-axis is (x,−y).
Image Point B′
Image of B(0,1) is B′(0,−1).
Tracing the Reflected Ray
The reflected ray passes through the point of incidence A(3,0) and the image point B′(0,−1).
Two-Point Form Equation
Equation of line through (x1,y1) and (x2,y2):
x−x1y−y1=x2−x1y2−y1
Using A(3,0) and B′(0,−1):
x−3y−0=0−3−1−0
Calculating the Slope
Slope m=−3−1=31
Equation becomes: x−3y=31
Final Equation
Cross-multiply to simplify:
3y=x−3
The Shortcut Method
Pro Tip: When reflecting across the x-axis (y=0), simply replace y with −y in the original equation.
Incident: x+3y=3
Reflected: x+3(−y)=3⟹x−3y=3
Rearranging: 3y=x−3
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The Sigma Insight: Various Forms of Equations of a Line
Solution Diagram
Analyzing the Setup
Imagine you are standing in a dark room, holding a laser pointer. You aim it at a mirror lying flat on the floor—the x-axis. As the beam hits the surface, it bounces off, obeying the fundamental law of reflection.
In the world of coordinate geometry, this is a beautiful dance of lines and points. Today, we are going to master the reflection of a ray of light defined by the equation x+3y=3.
The Collision
Every reflection begins with a collision. The ray travels through space until it meets the reflecting surface—the x-axis, which is defined by the equation y=0.
To find where our light ray strikes this mirror, we find the intersection of our line and the x-axis. By substituting y=0 into our incident ray equation:
x+3(0)=3
We immediately find that x=3. Thus, our point of incidence, A, is (3,0). This is the anchor point for our reflected ray.
The Virtual World
To find the path of the reflected ray, we use the Image Point Method. Imagine the space behind the mirror as a virtual world where the reflected ray behaves as if it originated from the virtual image of the incident ray.
We select a second point on the incident ray by setting x=0. Substituting this into x+3y=3, we get 3y=3, which simplifies to y=1. Thus, we have a second point, B(0,1).
The Mirror Transformation
The reflection of any point (x,y) across the x-axis (y=0) is simply (x,−y). The x-coordinate remains locked in place, while the y-coordinate flips its sign.
Applying this to our point B(0,1), we find its image B′ at (0,−1). This point B′ is our virtual source. The reflected ray must pass through both the point of incidence A(3,0) and this virtual image point B′(0,−1).
The Final Construction
We now define the reflected ray using the two points A(3,0) and B′(0,−1). Using the two-point form of a line equation:
x−x1y−y1=x2−x1y2−y1
Substituting our coordinates, we obtain:
x−3y−0=0−3−1−0
Simplifying the right side gives −3−1=31. Thus, x−3y=31. Cross-multiplying yields the final equation:
3y=x−3
The Pro Secret
In the high-pressure environment of the JEE Advanced, time is your most precious resource. When reflecting across the x-axis, you can simply replace y with −y in the original equation.
Starting with x+3y=3, replacing y with −y gives:
x+3(−y)=3⇒x−3y=3
Rearranging this, we get 3y=x−3. It is the exact same result, achieved in seconds. Keep this tool in your arsenal, but never forget the geometric beauty that makes it work.