The Dance of the Particle
Imagine a particle tracing a curved path in the xy-plane. We are given its position vector as a function of time: r(t)=2ti^−3t2j^. Our mission is to find its angular momentum about the origin at a specific moment, t=2 seconds.
Angular momentum, denoted by L, is a measure of the amount of rotation an object has, taking into account its mass, shape, and speed. For a point particle, it is elegantly defined by the cross product of its position vector r and its linear momentum p.
Mathematically, this is written as:
L=r×p=m(r×v)
Uncovering the Velocity
To use our master equation, we first need the velocity vector v. Velocity is simply the rate at which position changes with time. So, we differentiate the position vector r(t) with respect to t:
v=dtdr=dtd(2ti^−3t2j^)
Applying basic differentiation rules, we get:
v=2i^−6tj^
The Cross Product Execution
Now, we substitute our expressions for r and v into the angular momentum formula:
L=m[(2ti^−3t2j^)×(2i^−6tj^)]
Let's expand this cross product carefully. Remember the rules for unit vectors: the cross product of a vector with itself is zero (i^×i^=0, j^×j^=0). Also, i^×j^=k^ and j^×i^=−k^.
L=m[(2t)(2)(i^×i^)+(2t)(−6t)(i^×j^)−(3t2)(2)(j^×i^)−(3t2)(−6t)(j^×j^)]
L=m[0−12t2(k^)−6t2(−k^)−0]
L=m[−12t2k^+6t2k^]=−6mt2k^
The Final Calculation
We have a beautiful, simplified expression for the angular momentum at any time t. The problem asks for the value at t=2 seconds for a particle of mass m=2 kg. Let's plug these numbers in:
L=−6(2)(2)2k^
L=−12(4)k^=−48k^
Pro Tip: You could also substitute t=2 into r and v before taking the cross product.
At t=2, r=4i^−12j^ and v=2i^−12j^.
Then, L=2[(4i^−12j^)×(2i^−12j^)]=2[−48k^−(−24k^)]=2[−24k^]=−48k^. Both paths lead to the same elegant result!