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33 Experimental Researches of Characteristics of <strong>Wind</strong>rotor Models 185<br />

It is necessary to note also, that for all considered flow velocities the<br />

hydrotray rotors with controlled blades have self-started, while rotors with<br />

rigidly fixed blades must be spin upped, i.e., certain auxiliary torque M must<br />

be applied on the windrotor model shaft. Only after that a rotor continued<br />

rotation with constant revolution velocity.<br />

The dependencies Cp on Z for windrotor models with 2, 3, and 4 blades are<br />

presented in Fig. 33.1. It appeared, that the positional relationship of curves<br />

Cp(Z) for windrotor models with various numbers of blades essentially differ<br />

from that of similar curves for windrotor model with rigidly fixed blades.<br />

For the last, increasing number of blades leads to a shift of the right part of<br />

dome-shaped curve Cp(Z) to the left (i.e., reduces rapidity of a wheel), and<br />

on the contrary happens for windrotor models with controlled blades. Here<br />

the least high-speed has appeared for the rotor with 2 blades. The greatest<br />

values of both the operating ratio of flow energy Cp and the coefficient of<br />

windrotor torque Cm ware received just for the windrotor models with 3 and<br />

4 blades.<br />

The influence of the mechanism of windrotor blades control on the magnitude<br />

of the torque gained by a windrotor is especially great. The graphs<br />

Cm(Z) in Fig. 33.2 show that for both windrotor models with 3 and 4<br />

Cp<br />

0.15<br />

0.1<br />

0.05<br />

model N1<br />

4 bl.-fix.<br />

3 bl.-fix.<br />

2 bl.-fix.<br />

4 bl.- cont.<br />

3 bl.- cont.<br />

2 bl.- cont.<br />

0<br />

1.0 1.5 2.0 Z 2.5 3.0 3.5<br />

0.2<br />

0.15<br />

Cp<br />

0.1<br />

0.05<br />

model N2<br />

4 bl.-fix.<br />

3 bl.-fix.<br />

2 bl.-fix.<br />

4 bl.- cont.<br />

3 bl.- cont.<br />

2 bl.- cont.<br />

0<br />

0.5 1.0 Z 1.5 2.0<br />

Fig. 33.1. Dependencies of operation ratios of the flow energy Cp on coefficient of<br />

specific speed Z (flow velocity in hydrotray V =0.6ms −1 )<br />

Cm<br />

0.125<br />

0.1<br />

0.075<br />

0.05<br />

0.025<br />

model N1<br />

4 bl.-fix.<br />

3 bl.-fix.<br />

2 bl.-fix.<br />

4 bl.-cont.<br />

3 bl.-cont.<br />

2 bl.-cont.<br />

0<br />

1.0 1.5 2.0 Z 2.5 3.0 3.5<br />

Cm<br />

0.3<br />

0.25<br />

0.2<br />

0.15<br />

0.1<br />

0.05<br />

model N2<br />

4 bl.-fix.<br />

3 bl.-fix.<br />

2 bl.-fix.<br />

4 bl.-cont.<br />

3 bl.-cont.<br />

2 bl.-cont.<br />

0<br />

0.5 1.0 1.5 Z 2.0 2.5<br />

Fig. 33.2. Dependences of coefficients of windrotor model torque Cm on coefficient<br />

of specific speed Z (flow velocity in hydrotray V =0.6ms −1 )

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