What are the two questions on kinematics?

  • Thread starter Thread starter andrewhei
  • Start date Start date
  • Tags Tags
    Kinematics
andrewhei
Messages
5
Reaction score
0

Homework Statement



Q.1 A ball is thrown with speed v from the edge of acliff of height h. Assume that the ground below the cliff is horizontal. At what inclination angle should it be thrown so that it travels the maximum horizontal distance?

Q.2 An airplane has a speed of v and a range(out and home) of flight of Rin calm waether. Show that innorth blowing wind ofspeed w, it's range becomes (the eq. given below),in a direction whose true bearing is \theta.
Find the direction in which the range is maximum and the value of the maximum range.

Homework Equations



Q.1 2v2sin2\theta/g

Q.2 the given eq:
R' = R(v2 - w2)/v sqrt( v2 - w2 sin2 \theta )


The Attempt at a Solution



Q.1
I tried to divide it into two parts, the part above and the part below the cliff.
The Range for the part above the cliff is easy,which is 2v2sin2\theta/g .
But for the part below it, it's really complicated, I tried to do it but finding the time of flight by solving a quadtratic equation, then multiplying the horizontal component of the velocity to obtain the range.
When I add up the two parts, I diffrentiate the range with respect to theta, which gave me a very complicated equation that I can't solve for any values of theta.

Q.2
I tried to slove it by using relative velocity but I am getiing nowhere near the answer. Is there any other way?
 
Physics news on Phys.org
I've worked through part one and you will get a complicated looking equation for \Theta. I got:

(2(u\hat{}2) +2u)*sin\hat{}2(\Theta) + h*sin(\Theta) - 2u = 0

Where u is the initial velocity.

If you replace sin(\Theta) with x you can solve for x just like an ordinary quadratic. Then when you have your value for x, let's say you got x = 5, then you replace x with
sin(\Theta). So you have sin(\Theta) = 5. Then just solve for \Theta.
 
You need to use the kinematic equations to find the horizontal displacement in terms of the given quantities. Then maximize with respect to the angle of projection.

Kalvarin said:
I've worked through part one and you will get a complicated looking equation for \Theta. I got:

(2(u\hat{}2) +2u)*sin\hat{}2(\Theta) + h*sin(\Theta) - 2u = 0

Where u is the initial velocity.

Sorry, Kalvarin, but the above equation is dimensionally incorrect. You can't add u2 with u and h together. Also, what happened to g?
 
Yep, Kalvarin is wrong, but thanks for trying to help.
I solved question 1, finally, but I still can't solve question 2.
 
Hi, I had an exam and I completely messed up a problem. Especially one part which was necessary for the rest of the problem. Basically, I have a wormhole metric: $$(ds)^2 = -(dt)^2 + (dr)^2 + (r^2 + b^2)( (d\theta)^2 + sin^2 \theta (d\phi)^2 )$$ Where ##b=1## with an orbit only in the equatorial plane. We also know from the question that the orbit must satisfy this relationship: $$\varepsilon = \frac{1}{2} (\frac{dr}{d\tau})^2 + V_{eff}(r)$$ Ultimately, I was tasked to find the initial...
The value of H equals ## 10^{3}## in natural units, According to : https://en.wikipedia.org/wiki/Natural_units, ## t \sim 10^{-21} sec = 10^{21} Hz ##, and since ## \text{GeV} \sim 10^{24} \text{Hz } ##, ## GeV \sim 10^{24} \times 10^{-21} = 10^3 ## in natural units. So is this conversion correct? Also in the above formula, can I convert H to that natural units , since it’s a constant, while keeping k in Hz ?
Back
Top