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Question: A sphere of radius 10cm and mass \[{\mathbf{25}}{\text{ }}{\mathbf{kg}}\]is attached to the lower en...

A sphere of radius 10cm and mass 25 kg{\mathbf{25}}{\text{ }}{\mathbf{kg}}is attached to the lower end of steel wire of length 5 m{\mathbf{5}}{\text{ }}{\mathbf{m}}and diameter of 4 mm{\mathbf{4}}{\text{ }}{\mathbf{mm}}which is suspended from the ceiling of a room. The point of support is 521 cm{\mathbf{521}}{\text{ }}{\mathbf{cm}}above the floor. When the sphere is set swinging as a simple pendulum, its lowest point just grazes the floor. Calculate the velocity of the ball at its lowest position.

Explanation

Solution

As we know that when we apply a force on anybody there is some elongation and compression depending upon the situation. In this condition due to gravitational force there will be an elongation in the system due to which it will just graze the floor and continue its oscillatory motion. Formula for young’s modulus of elasticity (Y)=FLAΔL(Y) = \dfrac{{FL}}{{A\Delta L}} where FF is the applied force , LL is the length of wire, AA is the area of wire and ΔL\Delta L is the elongation in the wire.

Complete step by step solution:
We can get the following data clearly from the above question. Therefore, we can write:
Unstretched length of Steel wire (L) =500cm\left( L \right){\text{ }} = 500cm
Steel wire diameter (d) = 4mm = 0.4cm\left( d \right){\text{ }} = {\text{ }}4mm{\text{ }} = {\text{ }}0.4cm
Radius of the steel wire(R) =0.02cm\left( R \right){\text{ }} = 0.02cm
Mass of sphere = 25 kg = {\text{ }}25{\text{ }}kg
Radius of sphere =10 cm = 10{\text{ }}cm
Distance of floor from ceiling = 521 cm = {\text{ }}521{\text{ }}cm
Young’s modulus of elasticity for steel =2×1011 = 2 \times {10^{11}} N/m2N/{{\text{m}}^2}
Now, clearly from above we can write:
Total length of system before release = 500+ (10+10) =520cm = {\text{ }}500 + {\text{ }}\left( {10 + 10} \right){\text{ }} = 520cm
Due to gravitational force the elongation in wire () = 521cm  520 cm = 1 cm = 0.01m(){\text{ }} = {\text{ }}521cm{\text{ }}-{\text{ }}520{\text{ }}cm{\text{ }} = {\text{ }}1{\text{ }}cm{\text{ }} = {\text{ }}0.01m
On balancing the forces, we can write:
T=(mv2/R)+mgT = (m{v^2}/R) + mg (here R refers to the radius of arc that the system will follow i.e. 5m5mof string
+ 10 cm10{\text{ }}cmradius of sphere)
T=25v25.1+25×9.8 T=4.9v2+245  T = \dfrac{{25{v^2}}}{{5.1}} + 25 \times 9.8 \\\ T = 4.9{v^2} + 245 \\\
Now,

Y=FLAΔL ΔL=FLAY ΔL=FTAY  Y = \dfrac{{FL}}{{A\Delta L}} \\\ \Rightarrow \Delta L = \dfrac{{FL}}{{AY}} \\\ \Rightarrow \Delta L = \dfrac{{FT}}{{AY}} \\\
On putting the values the equation reduces as:
102=4.9v2+245)×5πd24×2×1011 102=(4.9v2+245)×53.14×(0.02)24×2×1011  {10^{ - 2}} = \dfrac{{4.9{v^2} + 245) \times 5}}{{\dfrac{{\pi {d^2}}}{4} \times 2 \times {{10}^{11}}}} \\\ \Rightarrow {10^{ - 2}} = \dfrac{{(4.9{v^2} + 245) \times 5}}{{\dfrac{{3.14 \times {{(0.02)}^2}}}{4} \times 2 \times {{10}^{11}}}} \\\

v=31m/sv = 31m/s

Note: At first visualize the problem and then proceed because many times the crux of the problem lies in its visualization.
Calculate tension and hence equate it to mv2+ mgm{v^2} + {\text{ }}mg.