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PhD Thesis (PDF) - Department of Astronomy - University of Virginia

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Pram ≈ 1.6 × 10 −11 dyne cm −2 . The ram pressure would be lower if NGC 1603 were<br />

at a larger radius than its projected radius (i.e., in front <strong>of</strong> or behind the center <strong>of</strong><br />

the NGC 1600 group). Roughly speaking, the condition for ram pressure to strip the<br />

gas is that Pram > Pgas, which appears plausible in the outer 4 ′′ –6 ′′ <strong>of</strong> NGC 1603.<br />

Since the tail points to the west towards the higher density gas near NGC 1600, the<br />

ambient gas density may have been higher in the past, making ram pressure stripping<br />

easier than it is at its present position.<br />

The NGC 1603 tail has a s<strong>of</strong>ter spectrum (Fig. 3.7, right) than the surrounding<br />

gas. Hardness ratios from counts in the same pie-shaped annuli used to construct<br />

Figure 3.8 confirm that the tail is s<strong>of</strong>ter in H21 by ≈2.6 σ. Thus, the jump in<br />

emission due to the tail is dominated by a jump in s<strong>of</strong>t emission, consistent with ram<br />

pressure stripping <strong>of</strong> cooler galactic gas by hotter group gas.<br />

NGC 1601 also has a velocity redshifted from NGC 1600 by ∼ 309 km s −1 , and its<br />

projected distance from NGC 1600 is only ∼28.5 kpc. Since the emission associated<br />

with NGC 1601 is fainter, its estimated thermal pressure is smaller than in NGC 1603.<br />

This, combined with its slightly higher velocity, suggests that ram pressure stripping<br />

should be stronger in NGC 1601 compared to NGC 1603. Although there is a hint <strong>of</strong><br />

a tail toward the east <strong>of</strong> NGC 1601 in Figure 3.7, it has only a 1.3 σ significance when<br />

the surface brightness in a hemispherical annulus east <strong>of</strong> NGC 1601 is compared with<br />

a similar annulus west <strong>of</strong> NGC 1601. There are a number <strong>of</strong> possible explanations <strong>of</strong><br />

why we do not see a significant tail around NGC 1601, while we see one for NGC 1603.<br />

First, NGC 1601 might have a small transverse velocity; the tail would then be<br />

projected onto NGC 1601 along our line <strong>of</strong> sight. In addition, the tail could be too<br />

faint, the projected velocity could be smaller than we estimated for NGC 1603, or<br />

projection effects could mean that NGC 1601 is actually in a lower density region in<br />

96

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