<p>It’s been 48 hours! I got my booklet back. For those of you who want to, let’s work out the solutions. I thought there were some interesting problems this year worth working out again.</p>
<p>I’ll start with Mechanics.</p>
<p>Mech 1.
a) Draw the forces on the block and slab.</p>
<p>I drew the weight and normal force on both the block and the slab. On the block, the frictional force pointed to the left; on the slab, it pointed to the right.</p>
<p>b) Calculate v_f.</p>
<p>a<em>b = F</em>f/M<em>b = (mu)(M</em>b)(g)/(M<em>b) = mu(g) = 1.96 m/s^2
a</em>s = F<em>f/M</em>s = (mu)(M<em>b)(g)/(M</em>s) = 0.327 m/s^2</p>
<p>v<em>b = v</em>0 - a<em>bt = 4.0 - 1.96t
v</em>s = 0 + a_st = 0.327t</p>
<p>v<em>f = v</em>b = v_s</p>
<p>4.0 - 1.96t = 0.327t
t = 1.75s</p>
<p>c) Calculate the distance the slab traveled when it reached v_f.</p>
<p>x = v_0<em>t + 1/2</em>a<em>t^2
x = 0 + 0.5</em>0.327*1.75^2
x = 0.501 m</p>
<p>d) Calculate the work done by friction on the slab.</p>
<p>F<em>f = mu*M</em>b<em>g = 0.98 N
W = F</em>d = 0.98 * 0.501 = 0.491 J</p>
<p>Mech 2.</p>
<p>a) Which quantities to graph?
Graph F on the y-axis and x^2 on the x-axis. The slope represents A.</p>
<p>b) Calculate values for the table.
Had to label the third column as “x^2 (m^2)”</p>
<p>The quantities were pretty self explanatory.
0.05 –> 0.0025
0.10 –> 0.0100
0.15 –> 0.0225
0.20 –> 0.0400
0.25 –> 0.0625</p>
<p>c) Plot the quantities in the table. Label axes.</p>
<p>Graph the points, draw a line of best fit.</p>
<p>d) Determine A.</p>
<p>Pick two points on the graph and find the slope. A would be somewhere between 1600 and 1750 N/m^2. I got 1670, personally.</p>
<p>e) Spring is now placed horizontally on the floor. Cart of mass 0.50 kg compresses spring 0.10m. Calculate the work done by the cart in compressing the spring to 0.10m.</p>
<p>W = int( F dx ) = int<a href=“1670x%5E2”>0, 0.10</a> = 0.557 J</p>
<p>f) Calculate the speed of the cart just before it hits the spring.</p>
<p>Conservation of energy.
U<em>i + K</em>i = U<em>f + K</em>f
0 + .5mv^2 = 0.557 + 0
.5(0.50)v^2 = 0.557
v = 1.49 m/s</p>
<p>Mech 3.
a) Derive an expression for the acceleration of the center of mass of the hoop.</p>
<p>(Note: Imagine that @ is theta and & is alpha.)</p>
<p>F = Mg sin @ - F<em>f
a = g sin @ - F</em>f/M</p>
<p>How to determine F_f? Friction exerts a torque on the hoop.</p>
<p>RF<em>f = I&
F</em>f = (MR^2)(a/R)/R
F_f = Ma</p>
<p>a = g sin @ - a
a = g sin @/2</p>
<p>b) Derive an expression for the speed of the center of mass of the hoop when it reaches the bottom of the ramp.</p>
<p>Conservation of energy, again!
U<em>i + K</em>i = U<em>f + K</em>f
Mg(L sin @) + 0 = 0 + .5Mv^2 + .5Iw^2
Mg(L sin @) = .5Mv^2 + .5(MR^2)(v/R)^2
MgL sin @ = .5Mv^2 + .5Mv^2
gL sin @ = v^2
v = sqrt(gL sin @)</p>
<p>c) Determine the horizontal distance from the table to where the hoop lands on the floor.</p>
<p>x = v*t
v = sqrt(gL sin @) <– all of the velocity is in the horizontal direction</p>
<p>H = v_0*t + .5at^2
t = sqrt(2H/g)</p>
<p>x = sqrt(gL sin @)*sqrt(2H/g)
x = sqrt(2HL sin @)</p>
<p>d) If the hoop is replaced by a disk, what will happen to the distance calculated in part (c).</p>
<p>Greater than. Because the rotational inertia of a disk is less than that of a hoop, the velocity when the disk reaches the bottom of the ramp will be greater than when the hoop reached the bottom. Therefore the disk will travel farther than the hoop.</p>