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Question: A block of mass 1 kg is released from P on a frictionless track which ends in quarter circular track...

A block of mass 1 kg is released from P on a frictionless track which ends in quarter circular track of radius 2 m at the bottom. What is the magnitude of radial acceleration and total acceleration of the block when it arrives at Q?

Explanation

Solution

Since the block is released from a certain height, so calculate the loss of height. We get the displacement of the object. Then by using the formula: v2=u2+2gs{{v}^{2}}={{u}^{2}}+2gs , find the final velocity of the block. Now, we know that the radial acceleration is given by: aR=v2r{{a}_{R}}=\dfrac{{{v}^{2}}}{r} and tangential acceleration is given by: aT=g{{a}_{T}}=g . So, total acceleration is: a=(aR)2+(aT)2a=\sqrt{{{\left( {{a}_{R}} \right)}^{2}}+{{\left( {{a}_{T}} \right)}^{2}}} .

Formula used:
v2=u2+2gs{{v}^{2}}={{u}^{2}}+2gs, where v is final velocity, u is initial velocity, g is the acceleration due to gravity and s is the distance covered.
aR=v2r{{a}_{R}}=\dfrac{{{v}^{2}}}{r}, where aR{{a}_{R}}is the radial acceleration, v is the velocity and r is the radius.
aT=g{{a}_{T}}=g, where aT{{a}_{T}} is the tangential acceleration and g is the acceleration due to gravity
a=(aR)2+(aT)2a=\sqrt{{{\left( {{a}_{R}} \right)}^{2}}+{{\left( {{a}_{T}} \right)}^{2}}}, where a is the total acceleration, aR{{a}_{R}}is the radial acceleration and aT{{a}_{T}} is the tangential acceleration.

Complete step by step answer:
We have:
h1=6m h2=2m u=0m/s m=1kg  {{h}_{1}}=6m \\\ {{h}_{2}}=2m \\\ u=0m/s \\\ m=1kg \\\
So, the displacement of the block is:
s=(62) s=4m \Rightarrow s=\left( 6-2 \right) \\\ \Rightarrow s=4m
Now, by using the Newton’s law of motion: v2=u2+2gs{{v}^{2}}={{u}^{2}}+2gs
We get:
v2=0+(2×9.81×4) v2=78.48m2s2 \Rightarrow {{v}^{2}}=0+\left( 2\times 9.81\times 4 \right) \\\ \Rightarrow {{v}^{2}}=78.48{{m}^{2}}{{s}^{-2}}
As we know that:
The radial acceleration is given by: aR=v2r{{a}_{R}}=\dfrac{{{v}^{2}}}{r}
So, we have:
aR=78.482 aR=39.2ms2 \Rightarrow {{a}_{R}}=\dfrac{78.48}{2} \\\ \Rightarrow {{a}_{R}}=39.2m{{s}^{-2}}
So, total acceleration is:
a=(aR)2+(aT)2 a=(39.2)2+(9.81)2 a=40.4ms2 \Rightarrow a=\sqrt{{{\left( {{a}_{R}} \right)}^{2}}+{{\left( {{a}_{T}} \right)}^{2}}} \\\ \Rightarrow a=\sqrt{{{\left( 39.2 \right)}^{2}}+{{\left( 9.81 \right)}^{2}}} \\\ \therefore a=40.4m{{s}^{-2}}

Note:
We have been given a block that is at rest and then it accelerates as it is released from the point P. The block is released from a certain height therefore its potential energy is converted into kinetic energy. So, by conserving the total energy, we can write:
ΔPE=ΔKE     mg(h2h1)=12m(v2u2)     (62)=12v2 78.48=v2 \Delta PE=\Delta KE \\\ \implies -mg\left( {{h}_{2}}-{{h}_{1}} \right)=\dfrac{1}{2}m\left( {{v}^{2}}-{{u}^{2}} \right) \\\ \implies \left( 6-2 \right)=\dfrac{1}{2}{{v}^{2}} \\\ \therefore 78.48={{v}^{2}}