Answer to Chapter 3
1. The resultant is 31m,
44° N of E. |
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2. (a) V1x =
-8.08, V1y = 0;
V2x = V2cos45° =
4.51cos45° = 3.19,
V2y = V2sin45° =
4.51sin45° = 3.19.
(b) For the components of
the resultant we have
Rx = V1x + V2x
= -8.08 + 3.19 = -4.89;
Ry = V1y + V2y
= 0 + 3.19 = 3.19.
We find the resultant from
R = (Rx2 + Ry2)1/2
= [(-4.89)2 + (3.19)2]1/2 = 5.84;
tan q = Ry/Rx =
(3.19)/(4.89) = 0.652, which gives
q = 33.1° above -x axis.
Note
that we have used the magnitude of Rx for the angle
indicated on the diagram
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3. (a) For the components we
have
Rx = Cx - Ax - Bx
= 0 - 66.0cos28.0° - (-40.0cos56.0°)
= -35.9;
Ry = Cy - Ay - By
= -46.8 -66.0sin28.0° - 40.0sin56.0°
= -111.0.
We find the resultant from
R = (Rx2 + Ry2)1/2
= [(-35.9)2 + (-111.0)2]1/2
= 117;
tan q = Ry/Rx = (111.0)/(35.9) = 3.09,
which gives
q =72.1° below -x
axis.
(b) For the components we have
Rx = 2Ax - 3Bx + 2Cx
= 2(66.0cos28.0°) - 3(-40.0cos56.0°) + 2(0)
= 183.8;
Ry = 2Ay - 3By + 2Cy
= 2(66.0sin28.0°) - 3(40.0sin56.0°) + 2(-46.8)
= -131.2.
We find the resultant from
R = (Rx2 + Ry2)1/2
= [(183.8)2 + (-131.2)2]1/2
= 266;
tan q = Ry/Rx =(131.2)/(183.8) = 0.714,
which gives
q =35.5° below +x axis.
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4. The horizontal velocity is constant,
and the vertical velocity will be zero when the pebbles hit the window.
Using the coordinate system shown, we find the vertical
component of the initial velocity from
vy2 = v0y2
+ 2a(h - y0)
0 = v0y2 + 2(-9.80m/s2)(8.0m
- 0), which gives v = 12.5m/s. which gives v0y
= 12.5m/s.
(We choose the
positive square root because we know that the pebbles are thrown upward.)
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We find the time for the pebbles to hit the window from the vertical
motion.
vy = v0y + at;
0 = 12.5m/s + (9.80m/s2)t, which gives t =
1.28s.
For the
horizontal motion we have
x = x0 + v0xt,;
9.0m = 0 + v0x(1.28s), which gives
v0x = 7.0m/s.
Because the
pebbles are traveling horizontally when they hit the window, this is their
speed.
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5. (a) At the highest point, the vertical velocity vy
= 0. We find the maximum height h from
vy2 = v0y2
+ 2ay(y - y0);
0 = [(75.2m/s)sin34.5°]2 + 2(-9.80m/s2)(h - 0),
which gives h =
92.6m.
(b) Because the
projectile returns to the same elevation, we have
y = y0 + v0yt + 1/2ayt2;
0 = 0 + (75.2m/s)(sin34.5°)t + 1/2(-9.80m/s2)t2,
which give t = 0, and 8.69s.
Because t = 0 was the launch time, the total time in the air
was 8.69s.
(c) We find the
horizontal distance from
x = v0xt = (75.2m/s)(cos34.5°)(8.69s)
= 539m.
(d) The
horizontal velocity will be constant: vx = vx0
= (75.2m/s)cos34.5° = 62.0m/s.
We find the vertical velocity from
vy = v0y + ayt =
(75.2m/s)sin34.5° + (-9.80m/s2)(1.50s) = 27.9m/s.
The magnitude of the velocity is
v = (vx2 + vy2)1/2
= [(62.0m/s)2 + (27.9m/s)2]1/2 = 68.0m/s.
We find the angle from
tan q = vy/vx = (27.9m/s)/(62.0m/s) = 0.450,
which gives q
=24.2° above the horizontal.
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