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If the linear density (mass per unit length) of a rod of length `3 m` is proportional to `x`, where `x`, where `x` is the distance from one end of the rod, the distance of the centre of gravity of the rod from this end is.

A

2.5 m

B

1 m

C

1.5 m

D

2 m

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The correct Answer is:
To find the distance of the center of gravity of a rod of length 3 m, where the linear density is proportional to the distance from one end, we can follow these steps: ### Step 1: Define the linear density We know that the linear density \( \lambda \) (mass per unit length) is proportional to the distance \( x \) from one end of the rod. We can express this as: \[ \lambda = kx \] where \( k \) is a constant of proportionality. ### Step 2: Determine the mass of an infinitesimal element Consider an infinitesimal element of the rod of length \( dx \) at a distance \( x \) from the end. The mass \( dm \) of this element can be expressed as: \[ dm = \lambda \cdot dx = kx \cdot dx \] ### Step 3: Set up the integrals for the center of mass The center of mass \( x_{cm} \) of the rod can be calculated using the formula: \[ x_{cm} = \frac{\int_0^L x \, dm}{\int_0^L dm} \] where \( L \) is the length of the rod (3 m in this case). ### Step 4: Calculate the numerator Substituting \( dm \) into the integral for the numerator: \[ \int_0^L x \, dm = \int_0^L x \cdot (kx \, dx) = k \int_0^L x^2 \, dx \] Calculating the integral: \[ \int_0^L x^2 \, dx = \left[ \frac{x^3}{3} \right]_0^L = \frac{L^3}{3} \] Thus, the numerator becomes: \[ k \cdot \frac{L^3}{3} \] ### Step 5: Calculate the denominator Now, we calculate the denominator: \[ \int_0^L dm = \int_0^L kx \, dx = k \int_0^L x \, dx \] Calculating this integral: \[ \int_0^L x \, dx = \left[ \frac{x^2}{2} \right]_0^L = \frac{L^2}{2} \] Thus, the denominator becomes: \[ k \cdot \frac{L^2}{2} \] ### Step 6: Substitute into the center of mass formula Now we can substitute the results from steps 4 and 5 into the center of mass formula: \[ x_{cm} = \frac{k \cdot \frac{L^3}{3}}{k \cdot \frac{L^2}{2}} = \frac{\frac{L^3}{3}}{\frac{L^2}{2}} = \frac{2L}{3} \] ### Step 7: Calculate the distance from the end Substituting \( L = 3 \, \text{m} \): \[ x_{cm} = \frac{2 \cdot 3}{3} = 2 \, \text{m} \] Thus, the distance of the center of gravity from one end of the rod is **2 meters**. ### Final Answer The distance of the center of gravity of the rod from the end is **2 meters**. ---

To find the distance of the center of gravity of a rod of length 3 m, where the linear density is proportional to the distance from one end, we can follow these steps: ### Step 1: Define the linear density We know that the linear density \( \lambda \) (mass per unit length) is proportional to the distance \( x \) from one end of the rod. We can express this as: \[ \lambda = kx \] where \( k \) is a constant of proportionality. ...
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