Oblio
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well, my c = vsin(theta)
The discussion focuses on deriving the trajectory of a projectile under the influence of gravity, specifically without air resistance. Participants clarify the integration process starting from Newton's second law, where the force of gravity is expressed as -mg = ma. The conversation emphasizes the importance of initial velocity components, particularly when considering angles, and how to integrate these components to find the position functions (x, y) over time. The final trajectory equation derived is y = (vsin(θ)x/cos(θ)) - (1/2)g x²/v²cos²(θ), which is essential for understanding projectile motion.
PREREQUISITESStudents and educators in physics, particularly those focusing on mechanics and projectile motion, as well as anyone involved in engineering applications requiring trajectory analysis.
Oblio said:well, my c = vsin(theta)
Oblio said:D=0... ?
Oblio said:0 = ma
C=v(x)
v(x) =vcos(theta), C=Vcos(theta)
y=v(x)t +D
y=D
at t=0, D=0 also.
Oblio said:algebraically or through another situation such as (t=0) (not that one I realize though)
Oblio said:nope. lol
Oblio said:ok, it asks for the trajectory as a function of x so:
y=vsin(theta)x/cos(theta) - (1/2)g x^2/v^2cos(theta)^2
learningphysics said:there should be vcos(theta) in the denominator in the first term.
Oblio said:sorry.
had that in ink ( i promise!)
Oblio said:I actually did that FIRST, thinking I was doing part a, but I actually did b.
I think this question is basically done, I can show you my other section maybe?
They do basically match.
Oblio said:y= (v_{yo} + v_{ter}x) / v_{xo} + v_{ter}\tau ln (1 - x / v_{xo}\tau)
I'll skip a simplification step unless its needed: Used taylor's series which allowed cancellations.
y=v_{yo}x / v_{xo} - x^2v_{ter}\tau / 2v_{xo}^{2}\tau^{2}