The linear mass density of a rod of length 2L varies with distance (x) from center as `lambda=lambda_(0)(1+(x)/(L))` .The distance of COM from center is nL.Then n is

If linear charge density of a wire of length L depends on distance x from one end as lambda=(lambda_(0)(x))/(L .Find total charge of wire :-

Linear mass density of a rod AB(of length 10 m) varies with distance x from its end A as lambda = lambda_0x^3 ( lambda_0 is positive constant) . Distance of centre of mass of the rod , from end B is

The linear mass density of a thin rod AB of length L varies from A to B as lambda (x) =lambda_0 (1 + x/L) . Where x is the distance from A. If M is the mass of the rod then its moment of inertia about an axis passing through A and perpendicualr to the rod is :

The linear mass density of a thin rod AB of length L varies from A to B as lambda (x) =lambda_0 (1 + x/L) . Where x is the distance from A. If M is the mass of the rod then its moment of inertia about an axis passing through A and perpendicualr to the rod is :

Linear mass density of a rod AB ( of length 10 m) varied with distance x from its end A as lambda = lambda_0 x^3 ( lamda_0 is poitive constant). Distance of centre of mass the rod, form end B is

Linear mass density of a rod AB ( of length 10 m) varied with distance x from its end A as lambda = lambda_0 x^3 ( lamda_0 is positive constant). Distance of centre of mass the rod, form end B is

the linear charge density of a thin metallic rod varies with the distance x from the end as lambda=lambda_(0)x^(2)(0 le x lel) The total charge on the rod is

the linear charge density of a thin metallic rod varies with the distance x from the end as lambda=lambda_(0)x^(2)(0 le x lel) The total charge on the rod is

The linear density of a rod of length L varies as rho=A+Bx where x is the distance from the left end. The distance of centre of mass from O is

The density of a thin rod of length l varies with the distance x from one end as rho=rho_0(x^2)/(l^2) . Find the position of centre of mass of rod.