First, we calculate the time for the projectile to stop and then we can get the maximum height:
V0=50smV(flight)=V0−gt⟹t=V0/gH(flight)=V0t−21gt2=t(V0−21gt)H(flight)=(V0/g)(V0−21V0)∴H(flight)=2gV02=2(9.81s2m)(50sm)2=127.42m
For the second part, we have to use the sum of external forces equal to the mass times the acceleration of the object, then we have two external forces: gravity and air resistance, we use this and the following operations to find the relation between velocity and height (we also have to consider that both forces have a negative sign because they are both against the movement of the projectile):
∑Fexternal=ma=−FD−mg=−(0.01mkg)V2−(10kg)g⟹a=dtdV=dydVdtdy⟹a=VdydV=−((0.001m−1)V2+g)∫V0V=0(0.001m−1)V2+gVdV=−∫y=0y=H(flight)dy[(0.002m−1)1ln((0.001m−1)V2+g)]V0V=0=−H(flight) H(flight)=−(500m)(ln(g)−ln(0.001V02+g))H(flight)=(500m)×ln(9.81)0.001(50)2+9.81=113.50m
Reference:
- Sears, F. W., & Zemansky, M. W. (1973). University physics.
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