The bar AB is pin-connected at one end to the slider at A and is pin-connected at the other end at B, which is on the disk D at the location shown. Disk D rolls without slipping over the horizontal surface. At the instant shown, slider A is moving in the direction shown with constant speed vo. At this instant, determine, as functions of R and vo, the angular velocities and angular accelerations of bar AB and disk D. 13 Answer AB ā AB Vo 2R R A AVO 11v² 72R² y 2R ·K, WD R B R R/2 Figure P16.128 Vo 3R D A k, a D = 119v²/ 108R2 k

The bar AB is pin-connected at one end to the slider at A and is pin-connected at the other end at B, which is on the disk D at the location shown. Disk D rolls without slipping over the horizontal surface. At the instant shown, slider A is moving in the direction shown with constant speed vo. At this instant, determine, as functions of R and vo, the angular velocities and angular accelerations of bar AB and disk D. 13 Answer AB ā AB Vo 2R R A AVO 11v² 72R² y 2R ·K, WD R B R R/2 Figure P16.128 Vo 3R D A k, a D = 119v²/ 108R2 k

Elements Of Electromagnetics

7th Edition

ISBN:9780190698614

Author:Sadiku, Matthew N. O.

Publisher:Sadiku, Matthew N. O.

ChapterMA: Math Assessment

Section: Chapter Questions

Problem 1.1MA

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Conservation of Energy

In physics, the rule of the conservation of energy states that energy doesn’t disappear from the atmosphere; instead, it changes its form from one type to another. Energy is one of the most important physical quantities in nature, and it cannot be created or destroyed — only transformed.

Question

Answers are provided

The bar AB is pin-connected at one end to the
slider at A and is pin-connected at the other end
at B, which is on the disk D at the location
shown. Disk D rolls without slipping over the
horizontal surface. At the instant shown, slider A
is moving in the direction shown with constant
speed vo. At this instant, determine, as functions
of R and vo, the angular velocities and angular
accelerations of bar AB and disk D.
▼ Answer
@
AB =
ā
AB
R
Vo
k,
2R
Avo
11v²/
72R²
y
13
-X
A
k,
2R
Figure P16.128
D
R
=
B
ส
à
R
R/2
Vo
k,
3R
D
D
119v²/
2
108R²
A
k

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