Conservation of Energy. Fountain Question

AI Thread Summary
The discussion centers on calculating the maximum height a fountain can lift a garbage can using principles of physics. One participant initially applies the conservation of energy, equating kinetic energy to potential energy, while another suggests using conservation of momentum for a more efficient solution. The latter approach simplifies the problem by setting the initial momentum to zero and equating it to the final momentum of the system, leading to a formula for maximum height. Both methods are deemed valid, but the momentum approach is highlighted for its efficiency. The conversation emphasizes the importance of understanding both energy and momentum principles in solving such problems.
mfianist
Messages
7
Reaction score
0
Water shoots up from a fountainat a speed of v0 at a rate of dm/dt, and hits a garbage can of mass M suspended in the air. What is the maximum height the fountain can lift the garbage can?

First i approached this problem with K.E = P.E

i assumed that m at time t = (dm/dt)t

so i put {M+(dm/dt)t}gh = 1/2 {(dm/dt)tv^2}

then i solved the equation for h.

i am not so sure if my approach is right...


Is there a better of solving this problem?
 
Physics news on Phys.org
Interesting problem. I was looking at this as an impulse problem. Recall the formula impulse P = Ft? So, assuming constant F, this gives us dP = Fdt for very small impulse bits. Rearrange and you have F = dP/dt, or, force equals the time derivative of momentum. Ah, momentum. So, what is the momentum of an object thrown upward as a function of its height? P=mv, so what is v as a function of h and some initial velocity v0? Find this P as a function of h, then find dP/dt keeping in mind dP = mdv + dmv and v is constant for a particular h. So, the garbage can has mass M, weighs Mg, it's force downward is its weight, where does the equivalent force upward come from?

This would probably be my approach, anyone see if I missed something obvious? I'm assuming inelastic collisions with the water particles, which seems reasonable.
 


Your approach is correct in using the conservation of energy principle, but there is a more efficient way to solve this problem. We can use the equation for the conservation of momentum, which states that the initial momentum of the system is equal to the final momentum of the system. In this case, the initial momentum is 0 as the garbage can is initially at rest, and the final momentum is (M + dm/dt)t * v0 as the garbage can is lifted by the water with a velocity of v0. Therefore, we can set these two equal to each other and solve for the maximum height h:

0 = (M + dm/dt)t * v0

h = (M + dm/dt)t * v0 / (M + dm/dt)g

This gives us the maximum height that the fountain can lift the garbage can, taking into account the rate of water flow. This approach is more efficient because it only involves one equation and does not require solving for multiple variables. However, your approach is also valid and will give the same result.
 
I multiplied the values first without the error limit. Got 19.38. rounded it off to 2 significant figures since the given data has 2 significant figures. So = 19. For error I used the above formula. It comes out about 1.48. Now my question is. Should I write the answer as 19±1.5 (rounding 1.48 to 2 significant figures) OR should I write it as 19±1. So in short, should the error have same number of significant figures as the mean value or should it have the same number of decimal places as...
Thread 'A cylinder connected to a hanging mass'
Let's declare that for the cylinder, mass = M = 10 kg Radius = R = 4 m For the wall and the floor, Friction coeff = ##\mu## = 0.5 For the hanging mass, mass = m = 11 kg First, we divide the force according to their respective plane (x and y thing, correct me if I'm wrong) and according to which, cylinder or the hanging mass, they're working on. Force on the hanging mass $$mg - T = ma$$ Force(Cylinder) on y $$N_f + f_w - Mg = 0$$ Force(Cylinder) on x $$T + f_f - N_w = Ma$$ There's also...
Back
Top