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The centre of mass of a non uniform rod ...

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)

A

(a) `(3/4)L`

B

(b) `(1/4)L`

C

(c) `(1/6)L`

D

(d) `(2/3)L`

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The correct Answer is:
To find the center of mass of a non-uniform rod of length \( L \) with a mass per unit length varying as \( \rho = \frac{kx^2}{L} \), we can follow these steps: ### Step 1: Define the mass element The mass element \( dm \) can be expressed in terms of the linear density \( \rho \) and an infinitesimal length \( dx \): \[ dm = \rho \, dx = \frac{kx^2}{L} \, dx \] ### Step 2: Set up the integral for the center of mass The center of mass \( x_{cm} \) is given by the formula: \[ x_{cm} = \frac{\int_0^L x \, dm}{\int_0^L dm} \] Substituting \( dm \) into the equation: \[ x_{cm} = \frac{\int_0^L x \left(\frac{kx^2}{L}\right) dx}{\int_0^L \left(\frac{kx^2}{L}\right) dx} \] ### Step 3: Calculate the numerator Now, we need to compute the numerator: \[ \int_0^L x \left(\frac{kx^2}{L}\right) dx = \frac{k}{L} \int_0^L x^3 \, dx \] Calculating the integral: \[ \int_0^L x^3 \, dx = \left[\frac{x^4}{4}\right]_0^L = \frac{L^4}{4} \] Thus, the numerator becomes: \[ \frac{k}{L} \cdot \frac{L^4}{4} = \frac{kL^3}{4} \] ### Step 4: Calculate the denominator Next, we compute the denominator: \[ \int_0^L \left(\frac{kx^2}{L}\right) dx = \frac{k}{L} \int_0^L x^2 \, dx \] Calculating the integral: \[ \int_0^L x^2 \, dx = \left[\frac{x^3}{3}\right]_0^L = \frac{L^3}{3} \] Thus, the denominator becomes: \[ \frac{k}{L} \cdot \frac{L^3}{3} = \frac{kL^2}{3} \] ### Step 5: Combine the results Now we can substitute the results back into the expression for \( x_{cm} \): \[ x_{cm} = \frac{\frac{kL^3}{4}}{\frac{kL^2}{3}} = \frac{L^3}{4} \cdot \frac{3}{kL^2} = \frac{3L}{4} \] ### Conclusion Thus, the center of mass of the non-uniform rod is located at: \[ x_{cm} = \frac{3L}{4} \]

To find the center of mass of a non-uniform rod of length \( L \) with a mass per unit length varying as \( \rho = \frac{kx^2}{L} \), we can follow these steps: ### Step 1: Define the mass element The mass element \( dm \) can be expressed in terms of the linear density \( \rho \) and an infinitesimal length \( dx \): \[ dm = \rho \, dx = \frac{kx^2}{L} \, dx \] ...
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DC PANDEY ENGLISH-CENTRE OF MASS, LINEAR MOMENTUM AND COLLISION-Level 1 Objective
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