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A rod is of length 3 m and its mass acti...

A rod is of length `3` m and its mass acting per unit length is directly proportional to distance x from its one end. The centre of gravity of the rod from that end will be at

A

1.5 m

B

2 m

C

2.5 m

D

3.0 m

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To find the center of gravity of a rod of length 3 m, where the mass per unit length is directly proportional to the distance from one end, we can follow these steps: ### Step-by-Step Solution: 1. **Define the Problem**: We have a rod of length \( L = 3 \) m. The mass per unit length \( \rho \) is directly proportional to the distance \( x \) from one end. This can be expressed as: \[ \rho(x) = kx \] where \( k \) is a constant of proportionality. 2. **Determine the Mass Element**: The mass of a small element \( dx \) of the rod at position \( x \) can be expressed as: \[ dm = \rho(x) \, dx = kx \, dx \] 3. **Set Up the Integral for Center of Mass**: The center of mass \( x_{cm} \) can be calculated using the formula: \[ x_{cm} = \frac{\int_0^L x \, dm}{\int_0^L dm} \] Substituting \( dm \): \[ x_{cm} = \frac{\int_0^3 x \cdot (kx \, dx)}{\int_0^3 (kx \, dx)} \] 4. **Calculate the Numerator**: The numerator becomes: \[ \int_0^3 x \cdot (kx) \, dx = k \int_0^3 x^2 \, dx = k \left[ \frac{x^3}{3} \right]_0^3 = k \cdot \frac{27}{3} = 9k \] 5. **Calculate the Denominator**: The denominator is: \[ \int_0^3 (kx) \, dx = k \left[ \frac{x^2}{2} \right]_0^3 = k \cdot \frac{9}{2} = \frac{9k}{2} \] 6. **Substitute Back into the Center of Mass Formula**: Now substituting the numerator and denominator into the center of mass formula: \[ x_{cm} = \frac{9k}{\frac{9k}{2}} = 9k \cdot \frac{2}{9k} = 2 \] 7. **Final Result**: Therefore, the center of gravity of the rod from the end where \( x = 0 \) is: \[ x_{cm} = 2 \text{ m} \]

To find the center of gravity of a rod of length 3 m, where the mass per unit length is directly proportional to the distance from one end, we can follow these steps: ### Step-by-Step Solution: 1. **Define the Problem**: We have a rod of length \( L = 3 \) m. The mass per unit length \( \rho \) is directly proportional to the distance \( x \) from one end. This can be expressed as: \[ \rho(x) = kx ...
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