Question #40894

A BLOCK SLIDES DOWN AN INCLINED PLANE OF SLOPE ANGLE THETA WITH A CONSTANT VELOCITY. IT IS THEN PROJECTED UP THE PLANE WITH AN INITIAL VELOCITY U. DISTANCE UPTO WHICH IT WILL RISE BEFORE COMING TO REST IS ?

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Answer on Question #40894 – Physics – Mechanics

A BLOCK SLIDES DOWN AN INCLINED PLANE OF SLOPE ANGLE THETA WITH A CONSTANT VELOCITY. IT IS THEN PROJECTED UP THE PLANE WITH AN INITIAL VELOCITY U. DISTANCE UPTO WHICH IT WILL RISE BEFORE COMING TO REST IS?

Solution:

Ffr\mathrm{F_{fr}} – friction force;

θ\theta – angle of the inclined plane;

U\mathrm{U} – initial velocity;

tt – time after the block stopped;

aa – deceleration of the block;

Newton’s second law for the block when it’s moving down along the X-axis before it was projected (V=constacceleration=0V = \text{const} \Rightarrow \text{acceleration} = 0):


x:Ffrmgx=0x: F_{fr} - mg_x = 0Ffr=mgxF_{fr} = mg_x


From the right triangle ABC:


sinθ=mgxmgmgx=mgsinθ\sin \theta = \frac{mg_x}{mg} \Rightarrow mg_x = mg \sin \theta


Newton’s second law for the block when it’s moving up along the X-axis after it was projected. Force that acts of the block:


x:Fnet=Ffr+mgxx: F_{net} = F_{fr} + mg_x


(1) and (2) in (3):


Fnet=mgx+mgx=2mgx=2mgsinθF_{net} = mg_x + mg_x = 2mg_x = 2mg \sin \theta


Loss of KE by block = work done by friction force + PE (final speed of the block = 0):


mU22=Fnetd+mgdsinθ\frac{mU^2}{2} = F_{net} \cdot d + mgd \cdot \sin \theta


(4) in (5):


mU22=2mgdsinθ+mgdsinθ\frac{mU^2}{2} = 2mgd \sin \theta + mgd \cdot \sin \thetaU22=3gdsinθ\frac {U ^ {2}}{2} = 3 \mathrm {g d} \sin \thetad=U26gsinθd = \frac {U ^ {2}}{6 g \sin \theta}


Answer: distance upto which block will rise before coming to rest is equal to U26gsinθ\frac{\mathrm{U}^2}{6\mathrm{g}\sin\theta} .

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