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A rigid body rotates about an axis throu...

A rigid body rotates about an axis through the origin with an angular velocity `10sqrt(3)`rad/s. If `omega` points in the direction of `hat(i)+hat(j)+hat(k)`, then the equation to the locus of the points having tangential speed 20m/s.

A

`x^(2)+y^(2)+z^(2)-xy-yz-xz-1=0`

B

`x^(2)+y^(2)+z^(2)-2xy-2yz-2xz-1=0`

C

`x^(2)+y^(2)+z^(2)-xy-yz-xz-2=0`

D

`x^(2)+y^(2)+z^(2)-2xy-2yz-2xz-2=0`

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The correct Answer is:
To solve the problem step by step, we will follow the given information and derive the equation for the locus of points with a specific tangential speed. ### Step 1: Determine the Angular Velocity Vector The angular velocity \( \omega \) is given as \( 10\sqrt{3} \) rad/s and points in the direction of \( \hat{i} + \hat{j} + \hat{k} \). To express \( \omega \) as a vector: 1. Find the unit vector in the direction of \( \hat{i} + \hat{j} + \hat{k} \): \[ \text{Magnitude of } (\hat{i} + \hat{j} + \hat{k}) = \sqrt{1^2 + 1^2 + 1^2} = \sqrt{3} \] Thus, the unit vector \( \hat{n} \) is: \[ \hat{n} = \frac{\hat{i} + \hat{j} + \hat{k}}{\sqrt{3}} \] 2. Now, express \( \omega \): \[ \omega = 10\sqrt{3} \cdot \hat{n} = 10\sqrt{3} \cdot \frac{\hat{i} + \hat{j} + \hat{k}}{\sqrt{3}} = 10(\hat{i} + \hat{j} + \hat{k}) = 10\hat{i} + 10\hat{j} + 10\hat{k} \] ### Step 2: Relate Tangential Speed to Angular Velocity The tangential speed \( v \) is given as 20 m/s. The relationship between tangential speed, angular velocity, and the position vector \( \mathbf{r} \) is given by: \[ \mathbf{v} = \omega \times \mathbf{r} \] where \( \mathbf{r} = x\hat{i} + y\hat{j} + z\hat{k} \). ### Step 3: Compute the Cross Product Using the values of \( \omega \) and \( \mathbf{r} \): \[ \mathbf{v} = (10\hat{i} + 10\hat{j} + 10\hat{k}) \times (x\hat{i} + y\hat{j} + z\hat{k}) \] Setting up the determinant for the cross product: \[ \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ 10 & 10 & 10 \\ x & y & z \end{vmatrix} \] Calculating this determinant: 1. For \( \hat{i} \): \[ \hat{i}(10z - 10y) = 10(z - y)\hat{i} \] 2. For \( \hat{j} \): \[ -\hat{j}(10z - 10x) = -10(z - x)\hat{j} \] 3. For \( \hat{k} \): \[ \hat{k}(10y - 10x) = 10(y - x)\hat{k} \] Thus, the velocity vector \( \mathbf{v} \) becomes: \[ \mathbf{v} = 10(z - y)\hat{i} - 10(z - x)\hat{j} + 10(y - x)\hat{k} \] ### Step 4: Find the Magnitude of the Velocity Vector The magnitude of \( \mathbf{v} \) is: \[ |\mathbf{v}| = \sqrt{(10(z - y))^2 + (-10(z - x))^2 + (10(y - x))^2} \] \[ = 10 \sqrt{(z - y)^2 + (z - x)^2 + (y - x)^2} \] ### Step 5: Set the Magnitude Equal to Tangential Speed Given that the tangential speed \( v = 20 \) m/s: \[ 20 = 10 \sqrt{(z - y)^2 + (z - x)^2 + (y - x)^2} \] Dividing both sides by 10: \[ 2 = \sqrt{(z - y)^2 + (z - x)^2 + (y - x)^2} \] ### Step 6: Square Both Sides Squaring both sides gives: \[ 4 = (z - y)^2 + (z - x)^2 + (y - x)^2 \] ### Step 7: Expand and Rearrange Expanding the right-hand side: \[ (z^2 - 2zy + y^2) + (z^2 - 2zx + x^2) + (y^2 - 2xy + x^2) = 4 \] Combining like terms: \[ 2z^2 + 2y^2 + 2x^2 - 2zy - 2zx - 2xy = 4 \] Dividing through by 2: \[ z^2 + y^2 + x^2 - zy - zx - xy = 2 \] ### Final Equation Thus, the equation of the locus is: \[ x^2 + y^2 + z^2 - xy - xz - yz - 2 = 0 \]
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