okay I see, then to get the change in internal energy ΔE = 1/2m(v+2u)2 - v2) = 2muv if you consider u << v, where (v+2u) is the velocity of the particle after the collision
Okay, but then for 2 b wouldn’t I get Δp = -8 - 2 = -10 Kgm/s, am i supposed to be getting Δp = 6 Kgm/s as this is -2mu = -2(1)(-3) as the question requires?
1
a) u = 2 ms-1v = -2ms-1
b) Δp = -2mu = -4 kgms-1
c) 0
d) F = dp/dt from Newton’s 2nd law, is it conserved because there’s and equal and opposite force acting on the hall by the wall ?
2
a) u = 2ms-1, v = -5 ms-1
b) -7 kgms-1
c) 22.5 J
3. -3 kgms-1
4. 22.5 J
i think v in 2 a is definitely...
So applying energy conservation in an elastic collision I’d have 1/2mv2 + 1/2Mu2 = 1/2mvf2 + 1/2Mu2 if I consider the energy of the piston too. Where vf is the final velocity of the particle. But then I’d get vf= v so that must be wrong
The advice made sense I just thought it only referred to the part of the question about momentum not internal energy, does the limit u <<v mean I need to use the binomial expansion since for kinetic energy you have v2, which in this case would be (v+u)2 ?
Here is the solution, I understand how they got E, but I don’t see how they could get E’ from cosine addition formulas? I don’t need to know how to do it with complex numbers.
I understand up to Asin(1+2cosφ). The max value of (1+2cosφ)^2 = 9 so you have to divide I0 by 9. I understand that now, but if the (1+2cosΦ) is the amplitude then the sinx must get averaged, but I thought that would introduce a factor of 1/2?