Galactic dust emission is concentrated in a bright band along the Galactic plane, with clumps associated with dust-rich regions. It is a foreground with a spectrum different from a 2.7 K blackbody, so multi-frequency observations can help separate it from the CMB. The schematic below illustrates its geometry rather than reproducing observed sky data.
Motion relative to an isotropic radiation field produces a dipole: one broad hot hemisphere and an opposite cool hemisphere. To first order T(θ)=T0[1+(v/c)cosθ], where θ=0 is the forward direction. This is not a narrow Galactic-plane feature and is not the intrinsic small-scale CMB pattern.
After foreground and dipole removal, primordial CMB anisotropies are small hot and cold patches across the sky, with characteristic correlated angular scales and amplitudes of order 10−5 of the mean temperature. They trace perturbations at photon decoupling and subsequent propagation, not simply the current distribution of Milky Way dust.
Expansion redshifts photon energies and preserves a blackbody spectrum, so a comoving observer at z=2 sees T=T0(1+z)≃8.18 K. A one-sided dipole excess of 0.105% means v/c=0.00105, hence v≃315 kms−1. Motion is toward the hotter region. The peak-to-peak contrast is twice this, so using 0.210% for v/c would double the inferred speed incorrectly.
The given calibration yields MV=−3.5log1050≃−5.946. The distance modulus is 31.446, giving d≃19.5 Mpc if extinction is negligible. Hubble's law predicts vH≃1400 km s−1, compared with 1150 km s−1 observed. The approximately −250 km s−1 difference can be a line-of-sight peculiar velocity of the cluster and observer, together with distance-calibration uncertainties. The local flow need not follow a perfectly smooth expansion law.
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