The Universe Is Expanding — Question 6

Section 44-10 · Physics pages 7482–7483

Question 6 Luminosity distance and angular distance answer different questions A source at z=1 has angular diameter distance DA = 1.5 Gpc. Assume photon conservation and DL = (1 + z)2DA. Its transverse size is 3.0 kpc. ℓ θ DA Schematic; labels, not drawing lengths, specify the data. (a) Find luminosity distance and angular size in radians. (b) If one wrongly used DA instead of DL in the flux law F = L/(4πD2 L), by what factor would the predicted flux be too large?
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Question 6 - Solution Luminosity distance and angular distance answer different questions ℓ θ DA (a) Method and calculation DL = 22(1.5) = 6.0 Gpc . θ = ℓ/DA = (3.0 × 103)/(1.5 × 109) = 2.0 × 10−6 rad . (b) Interpretation and further calculation Fwrong/Ftrue = D2 L/D2 A. Fwrong/Ftrue = 42 = 16 . Physical check The size is a proper transverse size at emission. Distance definitions converge nearby but differ substantially at high redshift.

Question 6

Luminosity distance and angular distance answer different questions

A source at z=1 has angular diameter distance DA=1.5D_A=1.5 Gpc. Assume photon conservation and DL=(1+z)2DAD_L=(1+z)^2D_A. Its transverse size is 3.0 kpc.

Diagram shown in the original SVG worksheet.

  1. Find luminosity distance and angular size in radians.

  2. If one wrongly used DA instead of DL in the flux law F=L/(4πDL2)F=L/(4\pi D_L^2), by what factor would the predicted flux be too large?

Question 6 - Solution

Luminosity distance and angular distance answer different questions

Diagram shown in the original SVG worksheet.

(a) Method and calculation

DL=22(1.5)=6.0Gpc.\boxed{D_L=2^2(1.5)=6.0\ {\mathrm{Gpc}}}.θ=ℓ/DA=(3.0×103)/(1.5×109)=2.0×10−6rad.\boxed{\theta=\ell/D_A=(3.0\times10^3)/(1.5\times10^9)=2.0\times10^{-6}\ {\mathrm{rad}}}.

(b) Interpretation and further calculation

Fwrong/Ftrue=DL2/DA2.F_{\mathrm{wrong}}/F_{\mathrm{true}}=D_L^2/D_A^2.Fwrong/Ftrue=42=16.\boxed{F_{\mathrm{wrong}}/F_{\mathrm{true}}=4^2=16}.

Physical check

The size is a proper transverse size at emission. Distance definitions converge nearby but differ substantially at high redshift.