Projectile Motion with Drag: Understanding F=ma and dv/dx in Physics

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SUMMARY

The discussion centers on the application of Newton's second law, F=ma, in the context of projectile motion with drag, specifically addressing the equation dv/dx = -gy - (bv/m). Participants clarify the distinction between dv/dt and dv/dx, emphasizing the importance of understanding potential energy in relation to work done against gravity. Additionally, the conversation shifts to the conversion of polar equations to Cartesian coordinates, highlighting the formulas x = rcos(θ) and y = rsin(θ) for conversion, and the challenges faced by students in grasping these concepts.

PREREQUISITES
  • Understanding of Newton's second law (F=ma)
  • Familiarity with drag force concepts (D = -bv)
  • Basic knowledge of polar and Cartesian coordinate systems
  • Ability to perform conversions between coordinate systems
NEXT STEPS
  • Study the implications of drag in projectile motion using differential equations
  • Learn about potential energy and work in physics
  • Practice converting between polar and Cartesian coordinates with various equations
  • Explore graphical representations of polar equations and their Cartesian counterparts
USEFUL FOR

Students in introductory physics courses, educators teaching mechanics, and anyone interested in mastering the concepts of motion, forces, and coordinate transformations.

Helena54321
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Hi First ever post on Physics Forum.

N2: F=ma can be written as dv/dx=-gy-(bv/m)

g=grav. constant
b=constant where D(total drag force opposing dir. of
trav.)=-bv
y is simply y/vertical component
m=mass

I know dv/dt=a but what is dv/dx-working with the units I just got m^2s^-1. Sooo please can anyone enlighten me on this? Just started uni nd this is in lecture notes.

Ahh merci x x x:blushing:
 
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Helena54321 said:
Hi First ever post on Physics Forum.

N2: F=ma can be written as dv/dx=-gy-(bv/m)

g=grav. constant
b=constant where D(total drag force opposing dir. of
trav.)=-bv
y is simply y/vertical component
m=mass

I know dv/dt=a but what is dv/dx-working with the units I just got m^2s^-1. Sooo please can anyone enlighten me on this? Just started uni nd this is in lecture notes.

Ahh merci x x x:blushing:
That should be dV/dx. The V stands for potential energy. If one does work against gravity, there is an increase in potential energy dV = -dW where W is work. F = -dV/dx follows from dV = -dW = -Fdx .

And, by the way, welcome to Physics Forums!

AM
 
Hi Andrew, thank you very much for replying to my post :). In the lecture the lecturer said that it was an error in the notes and it should be dv/dt.

I just did a test in another lecture and walked out crying. There was one question (which probably seems very easy to you :) ) were you had to convert polar equations to cartesian ones. We also had to draw the cartesian graphs (just 2D).

a) rcos(th)
b)r=2asin(th)
c)r^2sin2(th)=2k
d)rsin(th+(pi/4))=a2^(1/2)

th=theta.

In our lecture notes for this course we have derivations for conversion from cylindrical-cartesian (3D) and spherical-cylindrical. (-=either way)

But when it comes to 2D cartesian and polar I'm like ?. I have no clue what to do. I know a) is a straight line where x=a and b) is a circle but only because my friend told me.

I feel quite lost. How do I approach polar and cartesian egtn conversions?? Thank you.
 
Helena54321 said:
Hi Andrew, thank you very much for replying to my post :). In the lecture the lecturer said that it was an error in the notes and it should be dv/dt.

I just did a test in another lecture and walked out crying. There was one question (which probably seems very easy to you :) ) were you had to convert polar equations to cartesian ones. We also had to draw the cartesian graphs (just 2D).

a) rcos(th)
b)r=2asin(th)
c)r^2sin2(th)=2k
d)rsin(th+(pi/4))=a2^(1/2)

th=theta.

In our lecture notes for this course we have derivations for conversion from cylindrical-cartesian (3D) and spherical-cylindrical. (-=either way)

But when it comes to 2D cartesian and polar I'm like ?. I have no clue what to do. I know a) is a straight line where x=a and b) is a circle but only because my friend told me.

I feel quite lost. How do I approach polar and cartesian egtn conversions?? Thank you.
Polar co-ordinates are just another way of identifying a point on a plane. Rather than identifying the point by its position relative to the x and y axes, the point is identified by its displacement from the origin (distance and angle). You could give a position as "86.0 km east and 43.0 km north of the airport or you could say "97.5 km 30 degrees north of east of the airport".

To convert from polar to cartesian co-ordinates, x = r\cos\theta \text{ and }y = r\sin\theta. To go the other way:
r = \sqrt{x^2 + y^2)} \text{ and }\theta = \arctan (y/x).

Polar co-ordinates are useful for graphing relations that are symmetrical about the origin.

In cartesian co-ordinates, the equation for a circle is
y^2 = R^2 - x^2
but in polar co-ordinates it is just much simpler r = R (ie. r is constant).

To describe a straight line in the cartesian plane y = mx+b. In polar co-ordinates, it is not so easy unless it passes through the origin (ie \theta = constant).

As to your particular questions, a) is not an equation. But if rcos(th) = a, (for -\pi/2 < \theta < \pi/2) the graph would be a straight line x = a. Just do the conversion above. For the rest of them, plot a few points for each and see if you can visualize them and try to work them out using the above.

AM
 
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