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The angular momentum of a particle about...

The angular momentum of a particle about origin is varying as L =4t+8(SI units) whern its moves along a straight line y=x-4(x,y in metres). The magnitude of force acting on the particle will be

A

1 N

B

2 N

C

`sqrt2 N`

D

`sqrt3 N`

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The correct Answer is:
To solve the problem, we need to find the magnitude of the force acting on the particle given its angular momentum \( L \) and the path it follows. Let's break it down step by step. ### Step 1: Understanding Angular Momentum The angular momentum \( L \) of the particle about the origin is given by the equation: \[ L = 4t + 8 \] where \( t \) is time in seconds. ### Step 2: Finding the Rate of Change of Angular Momentum The torque \( \tau \) is defined as the rate of change of angular momentum: \[ \tau = \frac{dL}{dt} \] Calculating the derivative: \[ \frac{dL}{dt} = \frac{d}{dt}(4t + 8) = 4 \] Thus, the torque \( \tau \) is: \[ \tau = 4 \, \text{N m} \] ### Step 3: Analyzing the Particle's Motion The particle moves along the straight line given by the equation: \[ y = x - 4 \] This can be rewritten in standard form: \[ y - x + 4 = 0 \] The slope of this line is 1, which indicates that the angle \( \theta \) with respect to the x-axis is: \[ \tan \theta = 1 \implies \theta = 45^\circ \] ### Step 4: Relating Torque and Force The relationship between torque, force, and the position vector \( \mathbf{r} \) is given by: \[ \tau = \mathbf{F} \cdot \mathbf{r} \sin \theta \] In this case, since \( \theta = 45^\circ \): \[ \tau = F \cdot r \cdot \sin(45^\circ) \] We know that \( \sin(45^\circ) = \frac{1}{\sqrt{2}} \). ### Step 5: Solving for Force Rearranging the equation to solve for the magnitude of the force \( F \): \[ F = \frac{\tau}{r \cdot \sin(45^\circ)} \] Substituting \( \tau = 4 \, \text{N m} \) and \( \sin(45^\circ) = \frac{1}{\sqrt{2}} \): \[ F = \frac{4}{r \cdot \frac{1}{\sqrt{2}}} = \frac{4\sqrt{2}}{r} \] To find the magnitude of the force, we need the value of \( r \). ### Step 6: Finding the Position Vector \( r \) The position vector \( \mathbf{r} \) can be expressed in terms of \( x \) and \( y \). For the line \( y = x - 4 \), at any point \( (x, y) \): \[ r = \sqrt{x^2 + (x - 4)^2} = \sqrt{x^2 + (x^2 - 8x + 16)} = \sqrt{2x^2 - 8x + 16} \] However, we can simplify our calculations by noting that we need the force magnitude, which is independent of \( r \) in this case. ### Final Calculation Since we are looking for the magnitude of the force, we can conclude that: \[ F = 4 \sqrt{2} \text{ N} \] ### Conclusion Thus, the magnitude of the force acting on the particle is: \[ \boxed{4\sqrt{2} \, \text{N}} \]
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