 Quote by sorter
Same result too can be achieved using vortes generators such as wing fences on SU-22

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Those aren't vortex generators; they appear to besu-22 more closely related to something called a Gaster bump. The purpose of a Gaster bump is related to attachment line contamination rather than spanwise flow, as you will observe spanwise flow with or without such a device except very close to it.
Over the fuselage of a plane, the boundary layer is almost always turbulent before it even reaches the wing. On a wing, the turbulence continues from the wing root all the way down the attachment line, leading to early transition on the wing and a huge increase in drag. A Gaster bump prevents this from happening.
The fact that they extend so far back may be used to try and get rid of spanwise flow, but it is really only delaying the inevitable, as the pressure gradient alone on a swept wing will lead to spanwise flow.
 Quote by sorter
Why in the very 1st place spanwise airflow occurs i.e why not the air just flow straight towards the rear of wing?
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On a swept wing, you have two things that will help lead to spanwise flow. First, there is no leading edge stagnation point. Instead there is what is called an attachment line, which is essentially the linear analog. It shares everything in common with a stagnation point except there is a velocity along that leading edge of the wing away from the root. This means that as the air starts to flow over the wing, it starts out with some spanwise momentum.
The second reason is that on a swept wing, there is a pressure gradient that as a result of the sweep, tends to push the flow in the spanwise direction slightly.
 Quote by sorter
Is this spanwise airflow problem more prominent in Delta wing or Swept wing configuration?
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The phenomenon isn't really a problem, for starters. It also would be equally prevalent on a delta wing aircraft as it is on a swept wing aircraft provided they had the same sweep and airfoil. There isn't really an intrinsic preference for one design over the other.