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Two particles of mass m and 2m have thei...

Two particles of mass m and 2m have their position vectors as a function of time as `r_(1) (t) = hat i - t^(3) hat(j) +2t^(2)hat(k) and r_(2) (t) = t hat (i) -t^(3)hat(j) -t^(2) hatk` respectively (where t is the time). Which one of the following graphs represents the path of the centre of mass ?

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To find the path of the center of mass of two particles with given position vectors, we can follow these steps: ### Step 1: Identify the position vectors The position vectors of the two particles are given as: - For particle 1 (mass \( m \)): \[ \vec{r}_1(t) = \hat{i} - t^3 \hat{j} + 2t^2 \hat{k} \] - For particle 2 (mass \( 2m \)): \[ \vec{r}_2(t) = t \hat{i} - t^3 \hat{j} - t^2 \hat{k} \] ### Step 2: Write the formula for the center of mass The position vector of the center of mass \( \vec{r}_{cm} \) for two particles can be calculated using the formula: \[ \vec{r}_{cm} = \frac{m_1 \vec{r}_1 + m_2 \vec{r}_2}{m_1 + m_2} \] Where: - \( m_1 = m \) (mass of particle 1) - \( m_2 = 2m \) (mass of particle 2) ### Step 3: Substitute the values into the formula Substituting the masses and position vectors into the formula: \[ \vec{r}_{cm} = \frac{m \vec{r}_1 + 2m \vec{r}_2}{m + 2m} \] This simplifies to: \[ \vec{r}_{cm} = \frac{m \vec{r}_1 + 2m \vec{r}_2}{3m} \] \[ \vec{r}_{cm} = \frac{1}{3} \left( \vec{r}_1 + 2 \vec{r}_2 \right) \] ### Step 4: Calculate \( \vec{r}_{cm} \) Now, we will calculate \( \vec{r}_{cm} \): \[ \vec{r}_{cm} = \frac{1}{3} \left( \left( \hat{i} - t^3 \hat{j} + 2t^2 \hat{k} \right) + 2 \left( t \hat{i} - t^3 \hat{j} - t^2 \hat{k} \right) \right) \] Expanding this: \[ = \frac{1}{3} \left( \hat{i} - t^3 \hat{j} + 2t^2 \hat{k} + 2t \hat{i} - 2t^3 \hat{j} - 2t^2 \hat{k} \right) \] Combining like terms: \[ = \frac{1}{3} \left( (1 + 2t) \hat{i} + (-1 - 2)t^3 \hat{j} + (2 - 2)t^2 \hat{k} \right) \] This simplifies to: \[ = \frac{1}{3} \left( (1 + 2t) \hat{i} - 3t^3 \hat{j} \right) \] ### Step 5: Write the final expression for \( \vec{r}_{cm} \) Thus, the position vector of the center of mass is: \[ \vec{r}_{cm} = \frac{1 + 2t}{3} \hat{i} - t^3 \hat{j} \] ### Step 6: Analyze the components From the expression: - The x-component is \( \frac{1 + 2t}{3} \) which is always positive for \( t \geq 0 \). - The y-component is \( -t^3 \) which is always negative for \( t > 0 \). ### Step 7: Determine the path The path of the center of mass will be a curve where: - As \( t \) increases, the x-coordinate increases linearly, while the y-coordinate decreases cubically. ### Conclusion Based on the analysis, the graph representing the path of the center of mass will show a positive x-coordinate and a negative y-coordinate, indicating a curve that moves upwards to the right and downwards in the y-direction.
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