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Mechanics - 3B Scientific

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UE105060<br />

<strong>3B</strong> SCIENTIFIC® PHYSICS EXPERIMENT<br />

For the motions ϕ + = ϕ1 + ϕ2<br />

and ϕ − = ϕ1 − ϕ2<br />

(initially<br />

chosen arbitrarily) the equation of motion is as follows:<br />

L ⋅ ϕ&&<br />

L ⋅ ϕ&&<br />

+<br />

−<br />

+ g ⋅ ϕ<br />

+<br />

+<br />

The solutions<br />

ϕ<br />

ϕ<br />

+<br />

−<br />

= 0<br />

( g + 2k) ⋅ ϕ = 0<br />

= a cos<br />

+<br />

= a cos<br />

−<br />

−<br />

( ω+<br />

t) + b+<br />

sin( ω+<br />

t)<br />

( ω t) + b sin( ω t)<br />

−<br />

give rise to angular frequencies<br />

−<br />

−<br />

g<br />

g + 2k<br />

ω + = und ω − =<br />

(4)<br />

L<br />

L<br />

corresponding to the natural frequencies for in phase or out<br />

of phase motion (ϕ +<br />

= 0 for out of phase motion and ϕ –<br />

= 0<br />

for in-phase motion).<br />

The deflection of the pendulums can be calculated from the<br />

sum or the difference of the two motions, leading to the<br />

solutions<br />

1<br />

ϕ1<br />

=<br />

2<br />

1<br />

ϕ2<br />

=<br />

2<br />

( a cos( ω t) + b sin( ω t) + a cos( ω t) + b sin( ω t)<br />

)<br />

+<br />

( a cos( ω t) + b sin( ω t) − a cos( ω t) − b sin( ω t)<br />

)<br />

+<br />

+<br />

+<br />

+<br />

+<br />

+<br />

+<br />

Parameters a +<br />

, a –<br />

, b +<br />

and b –<br />

are arbitrary coefficients that<br />

can be calculated from the initial conditions for the two<br />

pendulums at time t = 0.<br />

The easiest case to interpret is where pendulum 1 is deflected<br />

by an angle ϕ 0 from its rest position and released at<br />

time 0 while pendulum 2 remains in its rest position.<br />

1<br />

ϕ1<br />

= ⋅<br />

2<br />

1<br />

ϕ2<br />

= ⋅<br />

2<br />

( ϕ ⋅ cos( ω t) + ϕ ⋅cos( ω t)<br />

)<br />

0<br />

+<br />

( ϕ ⋅ cos( ω t) − ϕ ⋅ cos( ω t)<br />

)<br />

0<br />

+<br />

0<br />

After rearranging the equations they take the form<br />

ϕ1<br />

= ϕ0<br />

⋅ cos<br />

ϕ = ϕ ⋅ sin<br />

2<br />

with<br />

0<br />

ω−<br />

− ω<br />

ω∆<br />

=<br />

2<br />

ω+<br />

+ ω−<br />

ω =<br />

2<br />

0<br />

( ω∆t) ⋅cos( ωt)<br />

( ω t) ⋅cos( ωt)<br />

+<br />

∆<br />

This corresponds to an oscillation of both pendulums at<br />

identical angular frequency ω, where the amplitudes are<br />

modulated at an angular frequency ω ∆ . This kind of modulation<br />

results in beats. In the situation described, the amplitude<br />

of the beats arrives at a maximum since the overall<br />

amplitude falls to a minimum at zero.<br />

−<br />

−<br />

−<br />

−<br />

−<br />

−<br />

−<br />

−<br />

−<br />

−<br />

(2)<br />

(3)<br />

(5)<br />

(6)<br />

(7)<br />

(8)<br />

LIST OF APPARATUS<br />

2 Pendulum rods with angle sensor U8404270<br />

1 Transformer 12 V, 2 A, e.g. U8475430<br />

1 Helical spring with two eyelets, 3 N/m U15027<br />

2 Table clamps U13260<br />

2 Stainless steel rods, 1000 mm U15004<br />

1 Stainless steel rod, 470 mm U15002<br />

4 Universal clamps U13255<br />

1 <strong>3B</strong> NETlog U11300<br />

1 <strong>3B</strong> NETlab for Windows U11310<br />

1 PC with Windows 98/2000/XP, Internet Explorer 6 or later,<br />

USB port<br />

SET-UP<br />

Fig. 2<br />

Set-up for recording and evaluating the oscillation of two<br />

identical pendulums coupled together by a spring<br />

The set-up is illustrated in Fig. 2.<br />

• Clamp two stand rods of 1000 mm length to a bench so<br />

that they are about 15 cm apart.<br />

• Attach a short stand rod between them as a horizontal<br />

cross member to lend the set-up more stability.<br />

• Attach the angle sensors to the top of the vertical rods<br />

using universal clamps.<br />

• Attach bobs to the end of the pendulum rods.<br />

• Suspend the pendulum rods from the angle sensors<br />

(there are grooves in the angle sensors to accommodate<br />

the hinge pins of the pendulum rods)<br />

2 / 5

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