Factors that affect the trajectory of a projected mass.

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SUMMARY

The discussion focuses on the factors affecting the trajectory of a projected mass, specifically highlighting the initial speed (u), initial height (h), gravitational constant (g), and angle of projection (θ). The participant utilized a ramp to manipulate the initial speed, deriving the formula v = √(2gH) for speed and t = √(2h/g) for time, leading to the horizontal displacement equation d = 2√(Hh). Key experimental discrepancies were attributed to air resistance and the coefficient of friction on the ramp, with clarification provided on the variable nature of air resistance relative to velocity.

PREREQUISITES
  • Understanding of basic physics concepts such as projectile motion and energy conservation.
  • Familiarity with mathematical equations related to motion, including kinematic equations.
  • Knowledge of forces acting on objects, specifically air resistance and friction.
  • Experience with experimental physics methods, particularly in measuring displacement and speed.
NEXT STEPS
  • Explore the effects of air resistance on projectile motion using computational simulations.
  • Investigate the relationship between the coefficient of friction and the efficiency of ramps in experiments.
  • Learn about rotational kinetic energy and its impact on the total energy of a system.
  • Study advanced projectile motion equations that incorporate air resistance for more accurate predictions.
USEFUL FOR

Students in physics courses, educators teaching projectile motion, and anyone interested in experimental physics and the dynamics of moving objects.

JMatch
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This is my physics coursework task and although I have had only minor difficulties in actually doing the work, I thought I would post some of the things that I found to verify.

Basically, I began with saying that the initial speed (u), initial height (h), gravitational constant (g) and the angle of projection (the) all played a role in determining the horizontal displacement (d) of the projected mass.

I varied the initial speed (u) by constructing a ramp and changing the vertical height of the mass 'up' the ramp (H). Keeping h, g constant and [tex]\theta[/tex] = 0, enabled me to find the initial speed as [tex]v = \sqrt{2gH}[/tex] (using conservation of energy).

I then found the time it would take for the mass to hit the floor, [tex]t = \sqrt{(2h)/g}[/tex] and combining this with the value for v enabled me to find out the horizontal displacement (d) in terms of H and h. [tex]d = 2\sqrt{Hh}[/tex]

That was the easy part. Deciding what factors made these theoretical results different from the experimental ones was a little harder.

Obviously air resistance will be a factor, as will the co-efficient of friction on the ramp. Those were the only two factors I could see that would make a difference.

I have a bit of a block when it comes to air resistance. I know I am wrong in thinking that air resistance is constant magnitude but varies in direction, however I am thinking it and it is annoying me.

Now I am forgetting the entire point of the task.. damn you PF!

(It should come to me soon, but any views so far?)
 
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If the mass was rolling down the ramp some of the potential energy would be converted to rotational kinetic energy.
 
JMatch said:
I have a bit of a block when it comes to air resistance. I know I am wrong in thinking that air resistance is constant magnitude but varies in direction, however I am thinking it and it is annoying me.

Now I am forgetting the entire point of the task.. damn you PF!

(It should come to me soon, but any views so far?)
The magnitude of air resistance isn't constant. It increases when the velocity increases and decreases when the velocity decreases. Unless you have a wind, the air resistance always opposes the direction of motion - i.e. relative to the object's motion, the direction of air resistance is always constant.
 

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