Simplifying Projectile Motion Equations

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Discussion Overview

The discussion revolves around the simplification of projectile motion equations, particularly focusing on the mathematical transformations involved and the implications of sign conventions for gravity in kinematic equations. Participants explore the relationships between horizontal and vertical components of motion, as well as the application of trigonometric identities.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested
  • Homework-related

Main Points Raised

  • One participant questions the simplification of the horizontal range equation, specifically the disappearance of the cosine term and its relation to trigonometric identities.
  • Another participant suggests that the identity \(\sin(2\theta) = 2\sin\theta\cos\theta\) is relevant to the simplification process.
  • There is a discussion about the sign of gravitational acceleration, with some participants asserting that gravity can be treated as negative or positive depending on the chosen coordinate system.
  • Participants express uncertainty about how to consistently apply the sign convention for gravity in projectile motion calculations.
  • One participant raises a question about the acceleration in the x-direction, leading to a clarification that in typical projectile motion problems, the x and y motions are independent, and the x-acceleration is often zero.
  • Another participant provides a specific problem involving a particle's motion in the xy-plane, expressing confusion about the x-acceleration and its implications for solving the problem.

Areas of Agreement / Disagreement

Participants generally agree on the importance of consistent sign conventions for gravity and the independence of x and y motion in projectile problems. However, there remains some uncertainty regarding the application of these concepts, particularly in relation to specific problems and the treatment of acceleration in the x-direction.

Contextual Notes

Some participants express limited knowledge of trigonometric identities, which may affect their understanding of the simplifications discussed. Additionally, there are unresolved questions regarding the application of kinematic equations in specific scenarios, particularly concerning the treatment of acceleration.

Who May Find This Useful

This discussion may be useful for physics students seeking clarification on projectile motion equations, trigonometric identities, and the application of sign conventions in kinematics.

leah3000
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referring to an object being projected upwards at an angle ө

i'm a phys student but i don't do math so I'm having trouble understanding how this equation has been simplified.

Horizontal Range= vcosө x 2vsinө/g

=v^2 2sinөcosө/g

this is the line i don't understand : v^2 sin^2 ө/g

where did the cosө go? is is a trig identity that cancels?:confused:

also when considering upward motion is g taken as negative?

if so, then why is the time taken to reach the maximum pt given by:

t= v sinө/ g wouldn't it be v sinө/ -g

isn't that the reason for the vertical distance traveled being given by;

y= v sinө t- 1/2 gt^2 ??
 
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Your intuition serves you well. I do think it was a trig identity that simplified your equation.

[tex]\sin\left( 2\theta\right)=2\sin\theta\cos\theta[/tex]

also, you are right again kind of... You can make your coordinate system any way you want, just as long as you're consistent. So make gravity negative but that formula you gave for time comes from this formula

[tex]v_{final}=at+v_{initial}[/tex]

and then setting the final velocity to zero, and inserting negative gravity

[tex]-v_{initial}=-gt[/tex]

and solving for time

[tex]\frac{v_{initial}}{g}=t[/tex]

note here in my work that
[tex]v\sin\theta = v[/tex]

So there gravity is positive, but that is because the negative signs canceled out left and right. This should get you your answers. So gravity can be negative, you just have to make sure to stay consistent once you decide how you want to orient yourself.
 
wow...thank you so much. It really did clear things up. I've never seen that identity before though...i have very limited knowledge of basic trigs lol

so then i should be specifying whether i use gravity as +ve/ -ve in general parabolic calculations?
 
leah3000 said:
wow...thank you so much. It really did clear things up. I've never seen that identity before though...i have very limited knowledge of basic trigs lol

so then i should be specifying whether i use gravity as +ve/ -ve in general parabolic calculations?

Yeah, so if you are going to call velocities and accelerations in the up direction positive, then gravity will be negative, but if you are going to call velocity and acceleration in the down direction positive, then gravity is positive, just make sure to follow whatever convention you set up right from the start. This is extremely important for kinematics! as you might have noticed ;)
 
i don't understand about why ax=o?
 
jfy4 said:
Yeah, so if you are going to call velocities and accelerations in the up direction positive, then gravity will be negative, but if you are going to call velocity and acceleration in the down direction positive, then gravity is positive, just make sure to follow whatever convention you set up right from the start. This is extremely important for kinematics! as you might have noticed ;)

this was very helpful...thank you so much:smile:
 
muaz89 said:
i don't understand about why ax=o?

It may very well be the case that [tex]a_{x}[/tex] is non-zero, and in that case, it must also be treated accordingly. Consider this, for all of these projectile motion problems, what happens in the x direction, has nothing to do with what happens in the y direction. The only link between these two directions is time. They both must match when it comes to how much time has past.

for most of these projectile problems, the acceleration [tex]a[/tex] and velocity [tex]v[/tex] can be broken down into their two x and y directions respectively

[tex]a_{x}=a\cos\theta[/tex] and [tex]a_{y}=a\sin\theta[/tex]

and [tex]v_{x}=v\cos\theta[/tex] and [tex]v_{y}=v\sin\theta[/tex]

These would comprise the velocity and accelerations found in almost any arbitrary projectile question, and the ability to break down a vector into its components is key for solving these problems.

So any problem could have an acceleration in the x direction, but i don't believe this is one of those cases, i think the projectile leaves at its trajectory at a constant [tex]v_{x}[/tex].
 
3 . A particle starts from the origin at t=0 with an initial velocity having an x-component of 20m/s and a y-component of -15m/s. The particle moves in the xy plane with an x component of acceleration only, given by ax = 4.0m/s2
a)Determine the total velocity vector at any time
b)Calculate the velocity and speed of the particle at t=0.5s
c)Determine the x and y coordinates of the particle at any time t and its position vector at this timewhat i know ax=o? so i m confused?
 
muaz89 said:
3 . A particle starts from the origin at t=0 with an initial velocity having an x-component of 20m/s and a y-component of -15m/s. The particle moves in the xy plane with an x component of acceleration only, given by ax = 4.0m/s2
a)Determine the total velocity vector at any time
b)Calculate the velocity and speed of the particle at t=0.5s
c)Determine the x and y coordinates of the particle at any time t and its position vector at this time


what i know ax=o? so i m confused?

[tex]a_{x}\not= 0[/tex] in this case, and their is no angle like i mentioned before.

I think the best approach for this problem would be to consider your velocity in terms of a vector and insert your acceleration vector into a kinematic equation.

[tex]v_{f}=at+v_{i}[/tex]

with your acceleration being [tex]a=4.0 \hat{i}[/tex] and your velocity being [tex]v_{i}=\left(20\hat{i}-15\hat{j}\right)[/tex].

putting these into the kinematic equation would give your total velocity for any time.

for the second part it is a matter of plugging in the time.

for the third part remember that the integral of velocity is position, so you can integrate your equation wrt time and solve for position.

this should point you in the right direction :)
 
  • #10
sorry for trouble you...:) .can you show the solution for all qeustion...because i dnt no so solve it...i very hope for you..
 

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