(a) We can calculate the initial momentum and this will be equal to the momentum at the end of the collision:
pi,T=m1v1,i+m2v2,i=m(v1,i+v2,i)pi,T=(6kg)[(−2m/s)+(0m/s)]pi,T=−12skg⋅m=pf,T (conservation of momentum)pf,T=m1v1,f+m2v2,f=m(v1,f+v2,f)−12skg⋅m=(6kg)[v1,f+v2,f]v1,f+v2,f=−2sm
Then, since the sum of the two velocities has to be equal to -2 m/s, this would mean that the kinetic energy is also conserved:
21mv1,i2=21mv1,f2+21mv2,f2⟹v1,i2=v1,f2+v2,f2
We can use the equation that relates the final velocities and elevate the whole expression to the square exponent and then we can have another equation that relates v1,f and v2,f:
\\ [v_{1,f}+v_{2,f}]^2= [-2\frac{m}{s}]^2
\\ \implies v^2_{1,f}+v^2_{2,f}+2v_{1,f}v_{2,f}=4\frac{m}{s^2}
Once we substitute on the equation that comes from the conservation of kinetic energy:
⟹v1,i2+2v1,fv2,f=4s2m2⟹(−2sm)2+2v1,fv2,f=4s2m24s2m2=2v1,fv2,f+4s2m→2v1,fv2,f=0s2m2
This last solution implies that one of the blocks has to stop moving while the other takes all the kinetic energy and starts traveling. In conclusion, we would suggest that m1 stopped moving while m2 started to move and then:
v1,f+v2,f=−2smsince v1,f=0sm;v2,f=−2smWith this we find the momentum:p2,f=mv2,f=(6kg)(−2sm)⟹p2,f=−12skg⋅m
Now, we only need to find the average net force applied if we know that for mass m2:
F=ΔtΔp=Δtpf−pi=0.05s−12skg⋅m−0skg⋅m ⟹F=240N
Reference:
- Sears, F. W., & Zemansky, M. W. (1973). University physics.
Comments