KE and U Energy in Spring Gun Question

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The discussion revolves around the mechanics of a child's spring gun, focusing on the spring constant, energy transfer, and the ball's launch dynamics. The key questions involve calculating the launch speed of the ball and determining the spring's initial compression distance. There is confusion regarding the final velocity at the ball's maximum height, with clarification needed on whether it should be zero. Participants also question the application of kinetic and potential energy equations, particularly regarding their components. The conversation emphasizes the importance of understanding energy conservation principles in this context.
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The spring in the muzzle of a child's spring gun has a spring constant of 730 N/m. To shoot a ball from the gun, first the spring is compressed and then the ball is placed on it. The gun's trigger then releases the spring, which pushes the ball through the muzzle. The ball leaves the spring just as it leaves the outer end of the muzzle. When the gun is inclined upward by 33° to the horizontal, a 50 g ball is shot to a maximum height of 1.75 m above the gun's muzzle. Assume air drag on the ball is negligible. (a) At what speed does the spring launch the ball? (b) Assuming that friction on the ball within the gun can be neglected, find the spring's initial compression distance.


i know how to solve it but my question is:

1/2 m (Vf^2 - Vi^2)= - mgh

the teacher put vf^2 = Vi cos 33

but I am wondering isn't Vf= 0 when it reaches the top??

Does KE and U energy have a components like forces??
 
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and for part b)
1/2 k x^2 = 1/2 mv^2
correct??
 
anyone??
 
Kindly see the attached pdf. My attempt to solve it, is in it. I'm wondering if my solution is right. My idea is this: At any point of time, the ball may be assumed to be at an incline which is at an angle of θ(kindly see both the pics in the pdf file). The value of θ will continuously change and so will the value of friction. I'm not able to figure out, why my solution is wrong, if it is wrong .
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