What changes could be made to a convex lense to produce an enlarged and upright image?
Distance of an object away from a concave mirror
Difference between images produced in concave/convex mirrors (between f and c)
Distinguishing between real and virtual images
Light shining through two slits and producing a pattern of multiple slits.
Sound heard walking past two speakers
The person walking in a straight line closer to the speakers will hear the loud and soft sounds at shorter distances as compared to the person walking in a straight line further away. This is because the antinodal lines fan out from the speakers, and therefore the further away one is from the speakers, the further apart the loud and soft sounds heard will be.
Find if point x is a node or antinode
Images formed by concave lenses
Regardless of the position of the object, the image will always be virtual, upright and diminished. The image is located on the object’s side of the lens.
Images formed by convex lenses
(Same as images formed in concave mirrors)
Images formed in concave mirrors
Images formed in convex mirrors
Regardless of the position of the object, the image will always be virtual, upright and diminished. The image is located behind the mirror.
Equation for critical angle
sinθc = n2 sin90°/n1
Where,
Total internal reflection
For total internal reflection to occur, the angle of incidence has to be greater than the critical angle, and the light ray must be travelling from a medium of a higher refractive index (optical density) to one of a lower refractive index.
Therefore, when rays of light at a very large angle of incidence hit the cold/hot air interface, the angle of incidence in greater than the critical angle, which causes all the light rays to undergo total internal reflection.
Critical angle
The critical angle is the angle of incidence (θ1), when the angle of refraction is 90°.
Refractive index
If two different mediums (water/air/glass) have different refractive indices, light will refract differently at the boundary between them.
When refraction occurs…
The frequency of the wave does not change when crossing the boundary. From v = fλ, velocity is directly proportional to wavelength. Therefore, as the frequency remains constant, and the wave velocity increases, the wavelength will increase also.
Refraction
Equation for path difference
with nodal lines
PS1 - PS2 = (n - 1/2) λ
Where,
Note - Nodal line number is taken from the central dotted line
Equation for path difference
with anti-nodal lines
PS1 - PS2 = nλ
Where,
Note - Antinodal line number is taken after the central dotted line (middle line = 0)
Diffraction
eg. Sound waves have a longer wavelength compared to light waves. Because of this longer wavelength, the soundwaves are more able to diffract around barriers (as the openings are around the same order of size as the wavelength of the sound waves). Comparatively, lightwaves cannot diffract as much around barriers. Therefore, often people can hear objects, but not see them.
Reflection and transmission of a pulse
Heavy string to light string
Heavy string to light string
Reflection and transmission of a pulse
Light string to heavy string
Light string to heavy string
Effect of adding an ammeter in parallel
Why bulb A in parallel will be brighter than bulb B if it has a higher resistance.