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Figure 5 shows four DASI images taken in the last 10 s of pump on for the cycle at 16 30 UT, from top to bottom, pump directions of −12°, −6°, vertical and +6° N. The +12° N position has not been included due to its similarity to +6° N. The red dotted lines in the left column of images show the position of the pump beam in 1° steps.
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This analysis method may be applied to other obliquely pumped schemes in which the pump direction does not parallel the axis of the resonator.
Advantages of the ETμP principle are the absence of any moving parts, force plateaus in broad frequency ranges, and a reversal of the pump direction in dependence on the driving frequency.
The consequence of this is that striations are saturated for all pumping directions, yet the optical emission intensity varies strongly with aspect angle.
Firstly, the two pumping directions are shown to give very different vortex structures, even though the flow numbers, Fl, are the same (=0.79).
The heat's pumping direction can be changed by altering the polarity of the charging DC current.
Twelve cases were studied by changing the direction of impeller rotation, impeller pumping direction, and the presence of baffles.
The main parameters considered were the impeller pumping direction (up versus down), impeller submergence, eccentricity, and angle of tilt.
The flow pattern and power number in a vessel depend on the impeller blade angle, number of blades, blade width, blade twist, blade thickness, pumping direction and interaction of flow with the vessel wall.
For northward pump beam directions, the optical emission intensity falls close to zero.
For pump beam directions further north from field aligned, the optical emission intensity decreases for the same pump power.
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