Concept:
The time period of a simple pendulum is given by:
\[
T = 2\pi \sqrt{\frac{l}{g
\]
where $l$ is the length of the pendulum and $g$ is the acceleration due to gravity.
Step 1: Condition in an orbiting laboratory
In an orbiting laboratory (such as a satellite), the system is in a state of free fall.
Although gravity still acts, both the pendulum and its support accelerate equally under gravity.
As a result, there is no effective restoring force, and the pendulum experiences weightlessness.
Thus, the effective gravitational acceleration becomes:
\[
g_{\text{eff = 0
\]
Step 2: Substitute into the time period formula
\[
T = 2\pi \sqrt{\frac{l}{g_{\text{eff
\]
As $g_{\text{eff \to 0$:
\[
T \to \infty
\]
Step 3: Physical interpretation
Since there is no restoring force acting on the bob, it does not oscillate.
Hence, the pendulum cannot execute periodic motion.
Conclusion:
\[
\boxed{T = \infty}
\]
The pendulum does not oscillate in an orbiting laboratory.