2. A particle moves along the curve \[ \begin{array}{l}x=2 t^{2}, \quad y=t^{2}-4 t \quad \text { and } \quad z=3 t-5 \\ \text { where } t \text { is the time. Find the components of its velocity and acceleration at time } t=1 \text {, in the } \\ \text { direction } \hat{i}-3 \hat{j}+2 \hat{k} \text {. } \\ \text { (Nagpur, Summer 200l) Ans. } \frac{8 \sqrt{14}}{7},-\frac{\sqrt{14}}{7}\end{array} \]
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To find the components of velocity and acceleration at time \( t = 1 \), we first differentiate the position functions. The velocity components are given by \[ \mathbf{v}(t) = \left( \frac{dx}{dt}, \frac{dy}{dt}, \frac{dz}{dt} \right) \] Taking derivatives, we have: - \( \frac{dx}{dt} = 4t \) - \( \frac{dy}{dt} = 2t - 4 \) - \( \frac{dz}{dt} = 3 \) At \( t = 1 \): - \( \mathbf{v}(1) = (4 \times 1, 2 \times 1 - 4, 3) = (4, -2, 3) \) Next, we find the acceleration by differentiating the velocity components: \[ \mathbf{a}(t) = \left( \frac{d^2x}{dt^2}, \frac{d^2y}{dt^2}, \frac{d^2z}{dt^2} \right) \] Calculating the second derivatives: - \( \frac{d^2x}{dt^2} = 4 \) - \( \frac{d^2y}{dt^2} = 2 \) - \( \frac{d^2z}{dt^2} = 0 \) Thus: - \( \mathbf{a}(1) = (4, 2, 0) \) Now, to find the components along the direction \( \hat{i} - 3 \hat{j} + 2 \hat{k} \), we normalize this vector: \[ \text{Magnitude} = \sqrt{1^2 + (-3)^2 + 2^2} = \sqrt{1 + 9 + 4} = \sqrt{14} \] The unit vector \( \mathbf{u} \) is: \[ \mathbf{u} = \left(\frac{1}{\sqrt{14}}, \frac{-3}{\sqrt{14}}, \frac{2}{\sqrt{14}}\right) \] Finally, the components of velocity and acceleration in the given direction are: - Velocity: \[ \mathbf{v} \cdot \mathbf{u} = \frac{4 \cdot 1 - 2 \cdot 3 + 3 \cdot 2}{\sqrt{14}} = \frac{4 - 6 + 6}{\sqrt{14}} = \frac{4}{\sqrt{14}} \] - Acceleration: \[ \mathbf{a} \cdot \mathbf{u} = \frac{4 \cdot 1 - 2 \cdot 3 + 0 \cdot 2}{\sqrt{14}} = \frac{4 - 6}{\sqrt{14}} = \frac{-2}{\sqrt{14}} \] The components at \( t = 1 \) are therefore: \[ \boxed{\left( \frac{4}{\sqrt{14}}, \frac{-2}{\sqrt{14}} \right)} \]