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However, maximum coolant temperature variation due to increased gap width is not changed by surface roughness.
The maximum coolant temperatures have sufficient margins to the sodium boiling point for all three unprotected transient scenarios.
The maximum cladding temperature, the maximum fuel center temperature and the maximum coolant velocity are all below the design constraints.
The maximum coolant pressure and surface heat flux capabilities are shown to be determined not only by the mechanical properties of the first wall material but also by the details of the blanket-design.
The thermal efficiency of the plant can be estimated using the maximum coolant temperature, and the capacity factor is derived from estimates of the planned and unplanned downtime, and the duty cycle if the reactor is pulsed.
The design criteria were restricted by the multiplication factor that should be less than 1.002, the average outlet coolant temperature 550 °C and the maximum coolant outlet temperature less than 700 °C.
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The reactor thermal power is 30 MW, and the reactor maximum outlet coolant temperature is 850 °C in rated operation mode and 950 °C in high-temperature test operation mode.
The blade diameter was about 200mm, and the maximum lead coolant flow rate in the course of the tests reached ∼2000 t/h.
The HTTR is a helium-cooled and graphite-moderated HTGR with a thermal power of 30 MW and a maximum reactor outlet coolant temperature of 950 °C.
The HTTR is the first HTGR in Japan with a thermal power of 30 MW and a maximum reactor outlet coolant temperature of 950 °C; it was built at the Oarai Research and Development Center of Japan Atomic Energy Agency JAEAAtomic Energy Agency JAEA
The general behavior of the reactor during LOEP is similar, but there are variations in important parameters such as flap valve open time, flow inversion time, and maximum fuel and coolant temperatures.
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