Yes. Suppose if we don't resolve the velocity, but if we resolve the field only, the component of field perpendicular to velocity will make the object move in a circle right ?
In both the ways we must see the object moving in a helix right. But in the second case I am seeing the particle moving in a tilted circular path... I think I am missing something
Yes. When you do diffraction problems they generally assume the distance to the screen is large compared to the distance between the slits. This is called the Fraunhofer limit. It simplifies the calculations in many ways.
I had a quick go at visualising the geometry involved but got tangled up and didn't get anywhere. It isn't priority to be honest since resolving the components of the velocity is the obvious way to do this.
@RonaldBecker I'd have to look at a particular example.
A horizontally oriented tube AB of length l rotates with a constant angular velocity ω about a stationary vertical axis OO’ passing through the end A (Fig. 1.86). The tube is filled with an ideal fluid. The end A of the tube is open, the closed end B has a very small orifice. Find the velocity of the fluid relative to the tube as a function of the column height h.
The problem with using Bernoulli's law is that in Bernoulli's law we generally use the gravitational acceleration 𝑔 and that's constant. Here we have the centripetal acceleration rω² and that changes with distance from the pivot.
If we move some mass of fluid 𝑚 from the inner surface of the liquid to the point B its PE changes due to the work done, and then if that mass squirts out from B the change in PE has to equal the change in KE. Yes?
As the angle changes during circular motion the initially parallel magnetic field component is no longer parallel and it will influence the trajectory I guess
Both branches have the same voltage across them. So whatever happens in one branch does not affect the other branch (assuming the power source is ideal). Yes?
So we remove branch 2 and then calculate the current in branch 1 using the same series phasor diagram that we are used to i.e. just the standard diagram with R on the x axis and +ωL on the y axis.
Now we go back to the original circuit and remove branch 1 leaving just branch 2. Again this does not affect the current in branch 2 so we can now use a standard phasor diagram with R₂ on the x axis and -1/ωC on the y axis.