Help quite hard pendulum problem

In summary, the conversation discusses the use of the parallel axis theorem and the calculation of the period of oscillation for a suspended rod and metre stick combination. The distance d, which is the perpendicular distance from the axis through the center of mass to the pivot, is determined to be the sum of the length of the rod and half the length of the ruler. The length L, which is used in the equation for the moment of inertia, refers to the length of the object with mass m, in this case the metre stick.
  • #1
charmedbeauty
271
0

Homework Statement



A very light rigid rod with a length of 0.062 m extends straight out from one end of a metre stick. The combination is suspended from a pivot at the upper end of the rod as shown in the following figure. The combination is then pulled out by a small angle and released.


Homework Equations





The Attempt at a Solution



well using parallel axis Theorem

I= 1/12mL2+md2

ω=√mgd/I

T=2∏/ω

T=2∏√(I/mgd)

= 2∏√((1/12)(m)(L)2+md2)/mgd

m's cancel

=2∏√((1/12)(L)2+d2)/gd

but what should d be??

is it a half L, I'm confused:confused:

is this the right method as well?
 
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  • #2
hi charmedbeauty! :smile:
charmedbeauty said:
A very light rigid rod with a length of 0.062 m extends straight out from one end of a metre stick. The combination is suspended from a pivot at the upper end of the rod as shown in the following figure.

but what should d be??

is it a half L, I'm confused:confused:

is this the right method as well?

looks ok :smile:

you're using the parallel axis theorem, and your axis through the c.o.m. is perpendicular to the rod, so d is the perpendicular distance from that axis to the pivot, ie the distance PC from the pivot P to the c.o.m. C

(if you're wondering how the moment of inertia can be the same whatever the angle θ of the stick, just do a bit of geometry using the cosine formula for two points A and B on the stick equidistant from C … you'll find that PA2 + PB2 is independent of θ :wink:)
 
  • #3
tiny-tim said:
hi charmedbeauty! :smile:


looks ok :smile:

you're using the parallel axis theorem, and your axis through the c.o.m. is perpendicular to the rod, so d is the perpendicular distance from that axis to the pivot, ie the distance PC from the pivot P to the c.o.m. C

(if you're wondering how the moment of inertia can be the same whatever the angle θ of the stick, just do a bit of geometry using the cosine formula for two points A and B on the stick equidistant from C … you'll find that PA2 + PB2 is independent of θ :wink:)

so say I have the pivot point which is connected to a rod which in turn is connected to a ruler then d would be the length of the the rod+half that of the ruler?? i.e. 0.5+0.062=d

http://www.webassign.net/serpse8/15-p-034-alt.gif

thats the pic there with all details given in question.
 
  • #4
charmedbeauty said:
so say I have the pivot point which is connected to a rod which in turn is connected to a ruler then d would be the length of the the rod+half that of the ruler?? i.e. 0.5+0.062=d

(oh it's straight!)

yes :smile:
 
  • #5
tiny-tim said:
(oh it's straight!)

yes :smile:
Thanks a bunch tiny-tim:approve:
 
  • #6
charmedbeauty said:
Thanks a bunch tiny-tim:approve:

and just to double check L is the length of the rod (0.062) and not the length of the ruler?
 
  • #7
no, L is in 1/12 mL2

L is the length of the thing that has mass m (in this case, the metre stick)
 
  • #8
tiny-tim said:
no, L is in 1/12 mL2

L is the length of the thing that has mass m (in this case, the metre stick)

oh right so I can just leave it out since it is 1 metre. cool.
 

FAQ: Help quite hard pendulum problem

What is a "quite hard pendulum problem"?

A "quite hard pendulum problem" refers to a complex physics problem that involves analyzing the motion of a pendulum, which is a weight suspended from a pivot point that swings back and forth. This type of problem is often difficult because it requires knowledge of various concepts such as gravity, motion, and energy.

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In a "quite hard pendulum problem", the pendulum is used as a model to understand the behavior of a system. It is typically used to represent a simple harmonic motion, where the pendulum's oscillatory motion can be described by a sine or cosine function.

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