The Cosmic Background Radiation — Question 8

Section 44-11 · Physics pages 7506–7507

Question 8 An acoustic angular scale combines a ruler with a distance In a supplied flat-cosmology model, the comoving sound horizon is 144 Mpc and the transverse comoving distance to last scattering is 13800 Mpc. Define θs = rs/DM and ℓA = π/θs. rs DM Schematic; labels, not drawing lengths, specify the data. (a) Calculate theta in radians and degrees, and the acoustic multipole scale. (b) If the sound horizon stays fixed but DM rises by 5 percent, find the fractional changes of theta and ellA.
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Question 8 - Solution An acoustic angular scale combines a ruler with a distance rs DM (a) Method and calculation θs = 144/13800 = .0104348 rad = .597869◦. ℓA = π(13800)/144 = 301.069 . (b) Interpretation and further calculation θ′ s/θs = 1/1.05 = .952381 . ℓ′ A/ℓA = 1.05 . Physical check The acoustic scale is not exactly the first temperature-peak multipole because phase shifts and detailed plasma dynamics affect peak locations.

Question 8

An acoustic angular scale combines a ruler with a distance

In a supplied flat-cosmology model, the comoving sound horizon is 144 Mpc and the transverse comoving distance to last scattering is 13800 Mpc. Define θs=rs/DM\theta_s=r_s/D_M and ℓA=π/θs\ell_A=\pi/\theta_s.

Diagram shown in the original SVG worksheet.

  1. Calculate theta in radians and degrees, and the acoustic multipole scale.

  2. If the sound horizon stays fixed but DM rises by 5 percent, find the fractional changes of theta and ellA.

Question 8 - Solution

An acoustic angular scale combines a ruler with a distance

Diagram shown in the original SVG worksheet.

(a) Method and calculation

θs=144/13800=.0104348rad=.597869∘.\boxed{\theta_s=144/13800=.0104348\ {\mathrm{rad}}=.597869^\circ}.ℓA=π(13800)/144=301.069.\boxed{\ell_A=\pi(13800)/144=301.069}.

(b) Interpretation and further calculation

θs′/θs=1/1.05=.952381.\boxed{\theta_s^\prime/\theta_s=1/1.05=.952381}.ℓA′/ℓA=1.05.\boxed{\ell_A^\prime/\ell_A=1.05}.

Physical check

The acoustic scale is not exactly the first temperature-peak multipole because phase shifts and detailed plasma dynamics affect peak locations.