<p>a. dv/dt = 1/t
dv = dt/t
v = ln(t) + C
-2 = ln(1) + C
C = -2
v(t) = ln(t) - 2</p>
<p>b. dx/dt = ln(t) - 2
dx = [ln(t) - 2]dt</p>
<p>We’ll want to integrate ln(t) by parts. udv = uv - ∫vdu
We’ll say that ln(t) = u and 1 = dv.</p>
<p>x = ln(t) * t - ∫(t/t)dt - 2t + C
x = tln(t) - t - 2t + C
x = tln(t) - 3t + C</p>
<p>4 = 1*ln(1) - 3(1) + C
4 = -3 + C
C = 7
x(t) = tln(t) - 3t + 7</p>
<p>c. When the particle is farthest to the left, the velocity is at a minimum. There is no relative minimum of the graph, but on the interval [1, ∞], the minimum exists at v(1). To find the position, we just plug into x(t). However, we’re already told that x(1) = 4, so good for us. The position of the particle is 4 units.</p>
<p>I’m an AB student who’s been reading ahead just for fun, so I hope that I did the integration by parts right (and for that matter, I hope I solved the problem correctly, hahaha).</p>