Home
Class 11
PHYSICS
The density of a non-uniform rod of leng...

The density of a non-uniform rod of length `1m` is given by `rho (x) = a (1 + bx^(2))`
where a and b are constants and `0 le x le 1`.
The centre of mass of the rod will be at

A

`(3(2 + b))/4(3 + b)`

B

`(4(2 + b))/3(3 + b)`

C

`(3(3 + b))/4(2 + b)`

D

`(4(3 + b))/3(2 + b)`

Text Solution

AI Generated Solution

The correct Answer is:
To find the center of mass of the non-uniform rod with the given density function, we can follow these steps: ### Step 1: Define the density function The density of the rod is given by: \[ \rho(x) = a(1 + bx^2) \] where \( a \) and \( b \) are constants, and \( 0 \leq x \leq 1 \). ### Step 2: Express the mass element The mass element \( dm \) can be expressed in terms of the density and a small length element \( dx \): \[ dm = \rho(x) \, dx = a(1 + bx^2) \, dx \] ### Step 3: Set up the center of mass formula The center of mass \( x_{cm} \) of the rod is given by the formula: \[ x_{cm} = \frac{\int_0^L x \, dm}{\int_0^L dm} \] where \( L \) is the length of the rod (1 meter in this case). ### Step 4: Calculate the numerator First, we need to calculate the integral for the numerator: \[ \int_0^1 x \, dm = \int_0^1 x \cdot a(1 + bx^2) \, dx \] This expands to: \[ \int_0^1 (ax + abx^3) \, dx \] Now, we can integrate term by term: \[ = a \int_0^1 x \, dx + ab \int_0^1 x^3 \, dx \] Calculating these integrals: \[ = a \left[ \frac{x^2}{2} \right]_0^1 + ab \left[ \frac{x^4}{4} \right]_0^1 \] \[ = a \cdot \frac{1}{2} + ab \cdot \frac{1}{4} = \frac{a}{2} + \frac{ab}{4} \] ### Step 5: Calculate the denominator Next, we calculate the integral for the denominator: \[ \int_0^1 dm = \int_0^1 a(1 + bx^2) \, dx \] This expands to: \[ = a \int_0^1 1 \, dx + ab \int_0^1 x^2 \, dx \] Calculating these integrals: \[ = a \left[ x \right]_0^1 + ab \left[ \frac{x^3}{3} \right]_0^1 \] \[ = a \cdot 1 + ab \cdot \frac{1}{3} = a + \frac{ab}{3} \] ### Step 6: Combine results to find the center of mass Now we can substitute the results from the numerator and denominator into the center of mass formula: \[ x_{cm} = \frac{\frac{a}{2} + \frac{ab}{4}}{a + \frac{ab}{3}} \] ### Step 7: Simplify the expression To simplify, we can multiply the numerator and denominator by 12 to eliminate the fractions: \[ x_{cm} = \frac{6a + 3ab}{12a + 4ab} \] This can be simplified further: \[ x_{cm} = \frac{3(2 + b)}{4(3 + b)} \] ### Final Result Thus, the center of mass of the rod is given by: \[ x_{cm} = \frac{3(2 + b)}{4(3 + b)} \]

To find the center of mass of the non-uniform rod with the given density function, we can follow these steps: ### Step 1: Define the density function The density of the rod is given by: \[ \rho(x) = a(1 + bx^2) \] where \( a \) and \( b \) are constants, and \( 0 \leq x \leq 1 \). ...
Promotional Banner

Topper's Solved these Questions

  • SYSTEM OF PARTICLES AND ROTATIONAL MOTIONS

    NCERT FINGERTIPS ENGLISH|Exercise ASSERTION AND REASON|15 Videos
  • SYSTEM OF PARTICLES AND ROTATIONAL MOTIONS

    NCERT FINGERTIPS ENGLISH|Exercise Kinematics Of Rotational Motion About A Fixed Axis|3 Videos
  • SYSTEM OF PARTICLES AND ROTATIONAL MOTIONS

    NCERT FINGERTIPS ENGLISH|Exercise HOTS HIGHER ORDER THINKING SKILL|8 Videos
  • PRACTICE PAPERS

    NCERT FINGERTIPS ENGLISH|Exercise All Questions|150 Videos
  • THERMAL PROPERTIES OF MATTER

    NCERT FINGERTIPS ENGLISH|Exercise Assertion And Reason|10 Videos

Similar Questions

Explore conceptually related problems

The linear density of a non - uniform rod of length 2m is given by lamda(x)=a(1+bx^(2)) where a and b are constants and 0lt=xlt=2 . The centre of mass of the rod will be at. X=

The centre of mass of a non uniform rod of length L, whose mass per unit length varies as rho=(k.x^2)/(L) where k is a constant and x is the distance of any point from one end is (from the same end)

The linear density of a thin rod of length 1m lies as lambda = (1+2x) , where x is the distance from its one end. Find the distance of its center of mass from this end.

A rod of length L is placed along the x-axis between x=0 and x=L . The linear mass density (mass/length) rho of the rod varies with the distance x from the origin as rho=a+bx . Here, a and b are constants. Find the position of centre of mass of this rod.

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) 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 centre of mass of a non-uniform rod of length L whose mass per unit length lambda is proportional to x^2 , where x is distance from one end

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

You are given a rod of length L. The linear mass density is lambda such that lambda=a+bx . Here a and b are constants and the mass of the rod increases as x decreases. Find the mass of the rod

If the linear mass density of a rod of length 3 m (lying from y=0 to y=3 m) varies as lambda =(2+y)kg/m,then position of the centre of mass of the rod from y=0 is nearly at