A torsion pendulum consists of a metal disk with a wire running through its center and soldered in place. The wire is mounted vertically on clamps and pulled taut. Figure 15-58 a gives the magnitude τ of the torque needed to rotate the disk about its center (and thus twist the wire) versus the rotation angle θ . The vertical axis scale is set by τ s = 4.0 × 10 -3 N ·m. The disk is rotated to θ = 0.200 rad and then released. Figure 15-58 b shows the resulting oscillation in terms of angular position θ versus time t . The horizontal axis scale is set by t s = 0.40 s. (a) What is the rotational inertia of the disk about its center? (b) What is the maximum angular speed d θ / dt of the disk? ( Caution: Do not confuse the (constant) angular frequency of the SHM with the (varying) angular speed of the rotating disk, even though they usually have the same symbol ω . Hint: The potential energy U of a torsion pendulum is equal to 1 2 k θ 2 , analogous to U = 1 2 kx 2 for a spring.) Figure 15-58 Problem 97
A torsion pendulum consists of a metal disk with a wire running through its center and soldered in place. The wire is mounted vertically on clamps and pulled taut. Figure 15-58 a gives the magnitude τ of the torque needed to rotate the disk about its center (and thus twist the wire) versus the rotation angle θ . The vertical axis scale is set by τ s = 4.0 × 10 -3 N ·m. The disk is rotated to θ = 0.200 rad and then released. Figure 15-58 b shows the resulting oscillation in terms of angular position θ versus time t . The horizontal axis scale is set by t s = 0.40 s. (a) What is the rotational inertia of the disk about its center? (b) What is the maximum angular speed d θ / dt of the disk? ( Caution: Do not confuse the (constant) angular frequency of the SHM with the (varying) angular speed of the rotating disk, even though they usually have the same symbol ω . Hint: The potential energy U of a torsion pendulum is equal to 1 2 k θ 2 , analogous to U = 1 2 kx 2 for a spring.) Figure 15-58 Problem 97
A torsion pendulum consists of a metal disk with a wire running through its center and soldered in place. The wire is mounted vertically on clamps and pulled taut. Figure 15-58a gives the magnitude τ of the torque needed to rotate the disk about its center (and thus twist the wire) versus the rotation angle
θ
. The vertical axis scale is set by τs = 4.0 × 10-3 N ·m. The disk is rotated to
θ
= 0.200 rad and then released. Figure 15-58b shows the resulting oscillation in terms of angular position
θ
versus time t. The horizontal axis scale is set by ts = 0.40 s. (a) What is the rotational inertia of the disk about its center? (b) What is the maximum angular speed d
θ
/dt of the disk? (Caution: Do not confuse the (constant) angular frequency of the SHM with the (varying) angular speed of the rotating disk, even though they usually have the same symbol
ω
. Hint: The potential energy U of a torsion pendulum is equal to
1
2
k
θ
2, analogous to U
=
1
2
kx2 for a spring.)
Figure 15-58 Problem 97
Definition Definition Special type of oscillation where the force of restoration is directly proportional to the displacement of the object from its mean or initial position. If an object is in motion such that the acceleration of the object is directly proportional to its displacement (which helps the moving object return to its resting position) then the object is said to undergo a simple harmonic motion. An object undergoing SHM always moves like a wave.
the cable may break and cause severe injury.
cable is more likely to break as compared to the
[1]
ds, inclined at angles of 30° and 50° to the vertical
rings by way of a scaled diagram. [4]
I
30°
T₁
3cm
3.8T2
cm
200 N
50°
at it is headed due North and its airspeed indicat
240 km/h. If there is a wind of 100 km/h from We
e relative to the Earth? [3]
Can you explain this using nodal analysis
With the nodes I have present
And then show me how many KCL equations I need to write, I’m thinking 2 since we have 2 dependent sources
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