00:01
So janet wants to find out the spring constant of a spring.
00:07
And to do this, she hangs a mass that's known, a mass that's given to us vertically, and measures the distance by which this mass drops from the spring.
00:22
So what's given to us here is the mass of this block, which is 0 .4 kilograms.
00:39
And we're given the distance by which it drops.
00:44
So we're going to write this distance here, and that distance is 3 cm or 0 .03 meters.
01:11
So in order to solve this problem, we need to see what's going on with our mass and our spring system.
01:21
It's hanging vertically, and the best thing we can start with is to draw a force diagram on this vertical system.
01:46
Okay, so our force diagram should include the following here.
01:55
We have m .g, the force of gravity, pulling the mass down.
02:02
We also have the restoring force, or in this case, i would say the spring force, acting opposite to the force of gravity, and that force is minus kx.
02:22
Now this box, or this mass spring system, is not oscillating.
02:28
It's not in simple harmonic motion, nor is the system accelerating.
02:34
So we know that a here, our acceleration is zero.
02:43
Since a is zero, our f net, our net force on this object has to be zero, in accordance with newton's second law of motion.
02:54
So, in our second step, we're going to invoke the second law of motion, and we're going to put together what we know and solve for the spring constant...