Surface stiffness optimization to improve morphing surface accuracy
US-11661184-B2 · May 30, 2023 · US
US2024199229A1 · US · A1
| Field | Value |
|---|---|
| Publication number | US-2024199229-A1 |
| Application number | US-202117908895-A |
| Country | US |
| Kind code | A1 |
| Filing date | Sep 7, 2021 |
| Priority date | May 24, 2021 |
| Publication date | Jun 20, 2024 |
| Grant date | — |
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A direct design method for generating an osculating curved waverider based on a complex leading edge, includes obtaining a leading edgeleading edge through determining a leading edge of a waverider according to a spread length, a front-to-rear length, and a sweep angle at each position of an aircraft, and arranging leading-edge discrete points on the leading edgeleading edge; drawing a small shock cone corresponding to each leading-edge discrete point by starting from each leading-edge discrete point, taking a local shock angle as a half cone angle and taking a free streamline direction as an axis; finding envelope surfaces of all small shock cones, namely, a shock curved surface corresponding to the leading edgeleading edge; generating a waverider by using the osculating curved waverider design method.
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1 . A direct design method for generating an osculating curved waverider based on a complex leading edge, comprising the steps of: step 1: obtaining a leading edgeleading edge through determining a leading edge of a waverider according to a spread length, a front-to-rear length, and a sweep angle at each position of an aircraft, and arranging leading-edge discrete points on the leading edgeleading edge; step 2: drawing a small shock cone corresponding to each leading-edge discrete point by starting from each leading-edge discrete point, taking a local shock angle as a half cone angle and taking a free streamline direction as an axis; step 3: finding envelope surfaces of all small shock cones, namely, a shock curved surface corresponding to the leading edgeleading edge; step 4: generating a waverider by using the osculating curved waverider design method. 2 . The direct design method for generating an osculating curved waverider based on a complex leading edge of claim 1 , wherein the method for obtaining the shock curved surface in step 3 further comprising the steps of: step 3-1: making the small shock cone obtained in step 2 intersect with a bottom plane perpendicular to the flow direction, thereby obtaining a series of bottom circles; subsequently, setting a i-th leading-edge discrete point to be P i (x i , y i , z i ), then a radius r i of the corresponding bottom circle being: r i =−x i tan β i , (1), wherein x i , y i , z i are the coordinates of the leading-edge discrete point and β i is the shock angle; step 3-2: drawing a common tangent circle of each three adjacent bottom circles, wherein center of the common tangent circle is a curvature center of an approximate conical flow field corresponding to the leading-edge discrete point, and a radius of the common tangent circle is a curvature radius of the approximate conical flow field; step 3-3: determining the approximate flow plane corresponding to the i-th leading-edge discrete point according to the i-th leading-edge discrete point, the corresponding common tangent circle center and the bottom circle center; step 3-4: connecting the i-th leading-edge discrete point with the tangent point of the corresponding common tangent circle and the bottom circle, thereby obtaining the i-th generatrix of the shock curved surface; step 3-5: going through all leading-edge discrete points by repeating steps 3-2 to 3-4, thereby obtaining the centers, radii, and tangent points of all common tangent circles corresponding to all leading-edge discrete points; step 3-6: connecting all generatrices obtained in step 3-4 into a ruled surface, namely, the shock curved surface corresponding to the leading edgeleading edge. 3 . The direct design method for generating an osculating curved waverider based on a complex leading edge of claim 2 , wherein in mathematics, drawing a common tangent circle of each three adjacent bottom circles belongs to Apollonius' problem, and the initial equation group is: { ( y - y 1 ) 2 + ( z - z 1 ) 2 = ( R - m r 1 ) 2 ( y - y 2 ) 2 + ( z - z 2 ) 2 = ( R - m r 2 ) 2 ( y - y 3 ) 2
Designing, manufacturing, assembling, cleaning, maintaining or repairing aircraft, not otherwise provided for; Handling, transporting, testing or inspecting aircraft components, not otherwise provided for · CPC title
Enabling technologies or technologies with a potential or indirect contribution to GHG emissions mitigation · CPC title
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