s i n ( θ 2 ) = 1.5 50 sin\Big(\dfrac{\theta}{2}\Big)=\dfrac{1.5}{50} s in ( 2 θ ) = 50 1.5
θ 2 = s i n − 1 ( 1.5 50 ) \dfrac{\theta}{2}=sin^{-1}\Big(\dfrac{1.5}{50}\Big) 2 θ = s i n − 1 ( 50 1.5 )
θ = 3.43 ° \theta=3.43\degree θ = 3.43°
Balancing forces in x direction,
T c o s ( 90 ° − 1.715 ° ) = F Tcos(90\degree-1.715\degree)=F T cos ( 90° − 1.715° ) = F
T = F c o s 88.28 ° ( 1 ) T=\dfrac{F}{cos88.28\degree}\space\space\space\space\space\space\space\space\space\space\space\space\space\space\space\space\space\space\space\space\space\space\space\space\space\space\space(1) T = cos 88.28° F ( 1 )
Balancing forces in y direction
T s i n 88.28 ° = m g Tsin88.28\degree=mg T s in 88.28° = m g
T = m g s i n 88.28 ° ( 2 ) T=\dfrac{mg}{sin88.28\degree}\space\space\space\space\space\space\space\space\space\space\space\space\space\space\space\space\space\space\space\space\space\space\space\space\space\space\space\space(2) T = s in 88.28° m g ( 2 )
From equation (1) and (2)
F m g = c o t 88.28 ° \dfrac{F}{mg}=cot88.28\degree m g F = co t 88.28°
F = m g × c o t 88.28 ° F=mg\times cot88.28\degree F = m g × co t 88.28°
F = 2.94 × 1 0 − 3 N F=2.94\times10^{-3}\space N F = 2.94 × 1 0 − 3 N
Let charges on both the sphere be q q q
Electrostatic force, F = k q 2 r 2 F=\dfrac{kq^2}{r^2} F = r 2 k q 2
q = ( 3 × 1 0 − 2 ) 2 ( 2.94 × 1 0 − 3 ) 9 × 1 0 9 q=\sqrt{\dfrac{(3\times10^{-2})^2(2.94\times10^{-3})}{9\times10^{9}}} q = 9 × 1 0 9 ( 3 × 1 0 − 2 ) 2 ( 2.94 × 1 0 − 3 )
q = 1.714 × 1 0 − 8 C q=1.714\times10^{-8}\space C q = 1.714 × 1 0 − 8 C
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