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A rod of length L and cross section area...

A rod of length L and cross section area A has variable density according to the relation `rho (x)=rho_(0)+kx` for `0 le x le L/2` and `rho(x)=2x^(2)` for `L/2 le x le L` where `rho_(0)` and k are constants. Find the mass of the rod.

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To find the mass of the rod with variable density, we will break the problem into two parts based on the given density functions for different segments of the rod. ### Step 1: Define the mass of the rod The mass \( m \) of the rod can be calculated using the formula: \[ m = \int \rho(x) \, dV \] where \( \rho(x) \) is the density at position \( x \) and \( dV \) is the differential volume element. For a rod with a cross-sectional area \( A \), the differential volume element can be expressed as \( A \, dx \). ### Step 2: Break the integral into two parts The rod is divided into two segments based on the given density functions: 1. From \( 0 \) to \( \frac{L}{2} \) where \( \rho(x) = \rho_0 + kx \) 2. From \( \frac{L}{2} \) to \( L \) where \( \rho(x) = 2x^2 \) Thus, we can write the mass as: \[ m = \int_0^{L/2} \rho_0 + kx \, A \, dx + \int_{L/2}^{L} 2x^2 \, A \, dx \] ### Step 3: Calculate the first integral For the first part of the rod: \[ m_1 = \int_0^{L/2} (\rho_0 + kx) A \, dx \] This can be separated into two integrals: \[ m_1 = A \left( \int_0^{L/2} \rho_0 \, dx + \int_0^{L/2} kx \, dx \right) \] Calculating each integral: 1. \(\int_0^{L/2} \rho_0 \, dx = \rho_0 \cdot \frac{L}{2}\) 2. \(\int_0^{L/2} kx \, dx = k \cdot \frac{(L/2)^2}{2} = \frac{kL^2}{8}\) Thus, we have: \[ m_1 = A \left( \rho_0 \cdot \frac{L}{2} + \frac{kL^2}{8} \right) \] ### Step 4: Calculate the second integral For the second part of the rod: \[ m_2 = \int_{L/2}^{L} 2x^2 \, A \, dx \] Calculating this integral: \[ m_2 = A \cdot 2 \int_{L/2}^{L} x^2 \, dx \] The integral \(\int x^2 \, dx\) is: \[ \int x^2 \, dx = \frac{x^3}{3} \] Evaluating from \(L/2\) to \(L\): \[ \int_{L/2}^{L} x^2 \, dx = \left[ \frac{L^3}{3} - \frac{(L/2)^3}{3} \right] = \frac{L^3}{3} - \frac{L^3}{24} = \frac{8L^3 - L^3}{24} = \frac{7L^3}{24} \] Thus: \[ m_2 = A \cdot 2 \cdot \frac{7L^3}{24} = \frac{7AL^3}{12} \] ### Step 5: Combine the masses Now, we can combine both parts to find the total mass of the rod: \[ m = m_1 + m_2 = A \left( \rho_0 \cdot \frac{L}{2} + \frac{kL^2}{8} \right) + \frac{7AL^3}{12} \] ### Final expression for the mass of the rod Thus, the total mass of the rod is: \[ m = A \left( \rho_0 \cdot \frac{L}{2} + \frac{kL^2}{8} + \frac{7L^3}{12} \right) \]

To find the mass of the rod with variable density, we will break the problem into two parts based on the given density functions for different segments of the rod. ### Step 1: Define the mass of the rod The mass \( m \) of the rod can be calculated using the formula: \[ m = \int \rho(x) \, dV \] where \( \rho(x) \) is the density at position \( x \) and \( dV \) is the differential volume element. For a rod with a cross-sectional area \( A \), the differential volume element can be expressed as \( A \, dx \). ...
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