364462 A pendulum made of a uniform wire of cross sectional area \(A\) has time period \(T\). When an additional mass \(M\) is added to its bob, the time period changes to \({T_M}\). If the Young's modulus of the material of the wire is \(Y\) then \(\dfrac{1}{Y}\) is equal to: \((g = \) gravitational acceleration\()\)
364462 A pendulum made of a uniform wire of cross sectional area \(A\) has time period \(T\). When an additional mass \(M\) is added to its bob, the time period changes to \({T_M}\). If the Young's modulus of the material of the wire is \(Y\) then \(\dfrac{1}{Y}\) is equal to: \((g = \) gravitational acceleration\()\)
364462 A pendulum made of a uniform wire of cross sectional area \(A\) has time period \(T\). When an additional mass \(M\) is added to its bob, the time period changes to \({T_M}\). If the Young's modulus of the material of the wire is \(Y\) then \(\dfrac{1}{Y}\) is equal to: \((g = \) gravitational acceleration\()\)
364462 A pendulum made of a uniform wire of cross sectional area \(A\) has time period \(T\). When an additional mass \(M\) is added to its bob, the time period changes to \({T_M}\). If the Young's modulus of the material of the wire is \(Y\) then \(\dfrac{1}{Y}\) is equal to: \((g = \) gravitational acceleration\()\)
364462 A pendulum made of a uniform wire of cross sectional area \(A\) has time period \(T\). When an additional mass \(M\) is added to its bob, the time period changes to \({T_M}\). If the Young's modulus of the material of the wire is \(Y\) then \(\dfrac{1}{Y}\) is equal to: \((g = \) gravitational acceleration\()\)