3: Waves Flashcards
(52 cards)
Progressive Wave
Waves, which transfer energy
Amplitude
The maximum displacement of a point on a wave from its rest position
Frequency
The amount of oscillations completed by a point on a wave per unit time
Wavelength
The length between two of the exact same points on a wave
Wave Speed
The speed at which waves travel
Wave Speed Formula
c = f λ
Frequency Formula
f = 1 / T
Longitudinal Waves
Waves where the direction of displacement of oscillating particles / fields is parallel to the direction of energy propagation
Transverse Waves
Waves where the direction of displacement of oscillating particles / fields is perpendicular to the direction of energy propagation
Phase
The fraction of a cycle that a point on a wave has completed since the start of that cycle
Phase Difference
Difference in phase between the exact same point on two waves measured in degrees, radians or fractions of a cycle
Polarisation
Where transverse waves are all oriented in the same direction – oscillating in the same plane (for EM waves, it is the electric fields, which can be polarised)
Applications of Polarisers (2)
- Polaroid material
- Alignment of aerials for transmission and reception
Polaroid material
A material, which polarises transverse waves (e.g., sunglasses)
Alignment of Aerials for Transmission & Reception (4)
- AC in transmitting aerial oscillates electromagnetic fields in one direction
- This produces a polarised EM waves
- EM waves oscillate electrons in receiving aerial producing the same frequency AC
- Transmitting and receiving aerials have to be aligned in the same orientation so that the waves are fully absorbed
Refractive Index of a Substance s
n = c / cₛ
n is refractive index of s
c is speed of light in vacuo in m s⁻¹
c is speed of light in s in m s⁻¹
Refractive Index of Air
~1
Refractive Index between Two Boundaries
₁n₂ = n₂ / n₁
₁n₂ is relative refractive index of a boundary (material 1 to material 2)
n₁ is refractive index of material 1
n₂ is refractive index of material 2
Snell’s Law of Refraction for a Boundary
n₁ sin θ₁ = n₂ sin θ₂
n₁ & n₂ are refractive indexes of materials 1 and 2
θ₁ is angle of incidence in °
θ₂ is angle of refraction in °
Total Internal Reflection (3)
When a ray travels from a more optically dense medium to a less, there will be a critical angle, θ. If:
- θᵢ < θ, there’s refraction and partial reflection
- θᵢ = θ, there’s refraction at 90° and partial reflection
- θᵢ > θ, there’s total reflection
Critical Angle Formula
sin θ = n₂ / n₁ for n₁ > n₂
θ is critical angle of boundary in °
n₁ & n₂ are refractive indexes of materials 1 and 2
Polarisation is Evidence for ____
The nature of transverse waves
Optical Fibres
A very thin tube of glass or plastic fibre, that can carry signals over long distances and round corners using total internal reflection
Step-Index Optical Fibres
Have a high refractive index core surrounded by low refractive index cladding to allow total internal reflection, which prevents light from escaping. The cladding also protects the core from scratches, which could allow light to escape