For this question I understand the markscheme but for part b when finding the displacement how is it possible that we can use both integration and SUVAT? I thought integration was only for variable acceleration and suvat had to be only for constant?
Suvat is when you integrate (differentiate) the constant acceleration case, so either use the formulae directly or (long way) integrate a constant acceleration so a <-> u + at <-> ut + 1/2 at^2 where you integrate/differentiate wrt t
Suvat is when you integrate (differentiate) the constant acceleration case, so either use the formulae directly or (long way) integrate a constant acceleration so a <-> u + at <-> ut + 1/2 at^2 where you integrate/differentiate wrt t
-So for constant acceleration you can use both integration/ differentiation and suvat its just quicker and preferred to use SUVAT ?
-but for variable acceleration questions you can only use integration/ differentiation ?
-So for constant acceleration you can use both integration/ differentiation and suvat its just quicker and preferred to use SUVAT ? -but for variable acceleration questions you can only use integration/ differentiation ?
Yes, suvat is simply the constant acceleration case where youve done the (definite) integral and the u,v are the velocity limits and 0,s are the displacement limits and 0,t the time limits.
For "interest", the time integration/differentiation case is straight forward so acceleration <-> velocity <-> displacement as in the previous post. The v - u = at suvat is simply change in momentum = impulse as multiplying through by m mv - mu = (ma)t so an applied force=ma over a time t (impulse) will produce a change in momentum mv-mu.
Similarly, the v^2 - u^2 = 2as can represent the conservation of energy as multiplying through by m/2 gives (1/2)mv^2 - (1/2)mu^2 = mas so a=g and s=h and you have change in KE = change in GPE. You can also derive it from the constant acceleration assumption as a = dv/dt = dv/ds ds/dt = v dv/ds and integrate (definite) both sides with respect to s you get as = (1/2) v^2 - (1/2) u^2
So the basic suvat equations can be relatively interesting if you make the links.
Yes, suvat is simply the constant acceleration case where youve done the (definite) integral and the u,v are the velocity limits and 0,s are the displacement limits and 0,t the time limits. For "interest", the time integration/differentiation case is straight forward so acceleration <-> velocity <-> displacement as in the previous post. The v - u = at suvat is simply change in momentum = impulse as multiplying through by m mv - mu = (ma)t so an applied force=ma over a time t (impulse) will produce a change in momentum mv-mu. Similarly, the v^2 - u^2 = 2as can represent the conservation of energy as multiplying through by m/2 gives (1/2)mv^2 - (1/2)mu^2 = mas so a=g and s=h and you have change in KE = change in GPE. You can also derive it from the constant acceleration assumption as a = dv/dt = dv/ds ds/dt = v dv/ds and integrate (definite) both sides with respect to s you get as = (1/2) v^2 - (1/2) u^2 So the basic suvat equations can be relatively interesting if you make the links.
Omg thank you that’s genuinely helped a lot and your right it is interesting especially as I take physics