Measurements were made of the flow structures in two types of spiral flow fields. The first was a vortex tube in which air entered one end of an 8-in. pipe through an involute entry and left a t the opposite end. The second was a conventional cyclone separator in which the same entry was used.The experimental results show that the mean and turbulent flow structures are not sensitive to changes in the flow rate, but,they are greatly affected by the geometry of the system. I n the vortex tube the angular velocity is nearly constant at radial distances less than one-half of the radius of the pipe. The flow patterns in the vortex tube and in the cyclone are not symmetrical with the pipe axis. The asymmetry can be explained by postulating a dynamic center line with helical shape. The longitudinal intensity of turbulence increases sharply near the center of the vortex tube. This is caused primarily by the abrupt decrease in mean velocity near the center. The radial intensity also increases near the center, but near the wall it decreases rapidly with distance from the center. The longitudinal intensity of turbulence in the cyclone is highest near the center and near the wall. The high intensity near the wall is caused bath by the decrease in mean velocity and the increase in root-mean-square turbulent velocity.Spiral flow is used in pulverized coal burners, flash vaporizers, cyclone separators, and other industrial equipment to promote mixing and to separate droplets and particles from gases. A better knowledge of the flow patterns and turbulence profiles in this type of flow should be useful in the design of industrial equipment. In this paper the mean flow patterns and components of the turbulence intensity and velocity products are reported for two types of spiral flow fields.A diagram of the flow system used is shown in Figure 1. The test section was an 8-in. pipe with the involute entrance shown in Figure 2. In one design the end of the pipe next to the entrance was closed, and the opposite end was open. This will be referred to as a "vortex tube." In the second design the end opposite the entrance was closed, and the exit piece shown in Figure 3 was installed next to the entrance to form a conventional cyclone separator.At points along the test section 5/16-in. holes were drilled through the pipe for insertion of ,the instruments used to measure the flow characteristics. The holes that were not in use when the measurements were being made were W. R. Schowalter is at princeton University, Princeton, New Jersey.plugged with modeling clay so that the inside of the pipe had a smooth surface. The location of the holes relative to the entrance is shown in Table 1.
MEASURING INSTRUMENTSThe pressure probe shown in Figure 4 was used with a hot-wire anemometer probe to find the direction of the mean velocity vector at points in the flow field.A constant-current hot-wire anemometer with a crossed-wire probe was used to measure U and the turbulent quantities (9, 10, 11, 1 3 ) . The probe was made of 0.00014 in. tungsten ...