Recent content by FallenLeibniz

  1. F

    Question about the relation b/w mean free path and other variables

    @Charles Link: I do thank you for your reply. It's much appreciated. I wasn't looking so much for the answer as the fact that setting the volumes equal could be just written down on paper enough. More or less, I was wondering the physical justification from behind the derivation. But, I do get...
  2. F

    Question about the relation b/w mean free path and other variables

    Homework Statement The problem that I am having stems from a problem given in the following way:[/B] "a)Show that for a gas, the mean free path ##\lambda## between collisions is related to the mean distance between nearest neighbors ##r## by the approximate relation ##\lambda \approx...
  3. F

    Basic Electric Field in Conductor Principles

    Homework Statement The following is a small concept exercise from an. EM text (Electromagnetism: Pollack and Stump). I believe I have the explanations correct, but am just looking for "peer-review" as they seem "hand-wavy": Suppose a conductor has a cavity inside it, and there is a point...
  4. F

    Motion on an inclined plane against a resisting force

    @andrewkirk : Figured it out. I kept looking at something wrong, but have seen the blood clot.
  5. F

    Motion on an inclined plane against a resisting force

    I was under the impression in my work that the resistive force would never be greater in magnitude than the effect of gravity. In my setup, $$k{v}^2$$ is the resistive acceleration and is pointing up the plane (in the positive x-direction) and $$g\sin(\theta)$$ points down the plane (in the...
  6. F

    Motion on an inclined plane against a resisting force

    @andrewkirk I am not sure what you mean by "you have distance x pointing up the plane". I did say that only my notion of what a "positive distance" was is going up the incline. Can you elaborate? @Student100 : I am attaching my work on the problem here...
  7. F

    Motion on an inclined plane against a resisting force

    Homework Statement I am trying to prove what is asked in the following problem: A particle of mass m slides down an inclined plane under the influence of gravity. If the motion is resisted by a ##f=kmv^2##, show that the time required to move a distance d after starting...
  8. F

    Moving body on an inclined plane

    Riiight. That makes more sense than the block jumping up in the air. Oops.
  9. F

    Moving body on an inclined plane

    After that don't you just square that velocity then divide by two times 9.8?
  10. F

    Moving body on an inclined plane

    Has anyone been able to get the answer that the OP says was correct? I have done this problem with both paradigms to try amd help them however I can not see how this answer of .35m is reached. Both ways give me that the mass hits at 3.597 m/s.
  11. F

    Moving body on an inclined plane

    Would you like kind enough to say what was wrong?
  12. F

    Equilibrium Position in Terms of Masses, Length, and Distance

    Here is the corrected equations list. I also want to thank the posters who have replied so far. I had been stuck on this for a really long time.
  13. F

    Equilibrium Position in Terms of Masses, Length, and Distance

    OK, so I took a look at my equations and there is something incorrect. The sum should be ##\vec{T_y}=\vec{T_a}+\vec{T_b}##. Furthermore the magnitudes of ##\vec{T_a}## and ##\vec{T_b}## are the same as the Tension (I believe a poster mentioned this above, but I didn't see what was meant till...
  14. F

    Equilibrium Position in Terms of Masses, Length, and Distance

    Yes,that wa Yes I do apologize. ##\vec{T}=\vec{Ta-Tb}## should be ##\vec{Ty}=\vec{Ta-Tb}##. My bad. I will update the equation list when I get back to my high tech white board . The above mentioned physics is still correct though right?
  15. F

    Equilibrium Position in Terms of Masses, Length, and Distance

    The force pair adds up to result in a vertical upward resultant force that counterbalances the weight of the second mass at equilibrium.
Back
Top