Visualization of the Poincaré sphere.
Showing how every fully polarized state of light can be represented by a point on a unit sphere. Linear polarization lies on the equator, circular polarization at the poles, and elliptical polarization everywhere in between. The sphere maps polarization states; it is not the physical path of light.
Showing how every fully polarized state of light can be represented by a point on a unit sphere. Linear polarization lies on the equator, circular polarization at the poles, and elliptical polarization everywhere in between. The sphere maps polarization states; it is not the physical path of light.
This media is not supported in your browser
VIEW IN TELEGRAM
This media is not supported in your browser
VIEW IN TELEGRAM
Visualization of Hanson’s n = 4 Fermat-quartic construction, z₁⁴ + z₂⁴ = 1.
Sixteen complex patches assemble into a genus-three surface in ℂ² ≅ ℝ⁴ before being projected into the three-dimensional form we can see. Its apparent self-intersections arise from losing one dimension during projection, they are not intersections in the original surface.
This is a mathematically exact slice associated with a quartic K3 surface, not an image of an entire Calabi–Yau manifold.
Sixteen complex patches assemble into a genus-three surface in ℂ² ≅ ℝ⁴ before being projected into the three-dimensional form we can see. Its apparent self-intersections arise from losing one dimension during projection, they are not intersections in the original surface.
This is a mathematically exact slice associated with a quartic K3 surface, not an image of an entire Calabi–Yau manifold.
🤔1
Hey I guess it's time back to get relevant and start solving
Question
Mains highly relevant stuff
I stand with dropper gang 12th waalo woh apna dekh le 💪🔥🔥
[ noob dropper gang ]
Now Competition badha denge dropper waale
Question
Mains highly relevant stuff
I stand with dropper gang 12th waalo woh apna dekh le 💪🔥🔥
[ noob dropper gang ]
Now Competition badha denge dropper waale
👍4🤯1👌1
Visualization of Lissajous figures.
Showing how two independent, perpendicular harmonic oscillations combine into a single geometric trace.
x(t) = A sin(mωt + δ)
y(t) = B sin(nωt)
Integer frequency ratios such as 1:1, 2:1, 3:2 and 5:4 produce closed repeating curves. Their relative phase controls whether the 1:1 pattern becomes a line, ellipse or circle, while an irrational ratio such as 1:√2 never closes exactly.
These are not arbitrary decorative patterns. They are the trajectory of the point (x(t), y(t)) and can be produced physically on an oscilloscope operating in X–Y mode.
Showing how two independent, perpendicular harmonic oscillations combine into a single geometric trace.
x(t) = A sin(mωt + δ)
y(t) = B sin(nωt)
Integer frequency ratios such as 1:1, 2:1, 3:2 and 5:4 produce closed repeating curves. Their relative phase controls whether the 1:1 pattern becomes a line, ellipse or circle, while an irrational ratio such as 1:√2 never closes exactly.
These are not arbitrary decorative patterns. They are the trajectory of the point (x(t), y(t)) and can be produced physically on an oscilloscope operating in X–Y mode.
This media is not supported in your browser
VIEW IN TELEGRAM
❤1
14_RA(Optional)_Geometrical_Optics_Eng.pdf
16.4 MB
14_RA(Optional)_Geometrical_Optics_Eng.pdf
So yes optics questions
So yes optics questions
❤2