Your question is great! Before answering your question, I would like to visualize some concepts for you:

We consider the **Riemann tensor** first. A crucial observation is that if we parallel
transport a vector $u$ at $p$ to $q$ along two different pathes $vw$ and $wv$, the resulting
vectors at $q$ are different in general (following figure). If, however, we parallel transport
a vector in a Euclidean space, where the parallel transport is defined in our
usual sense, the resulting vector does not depend on the path along which it
has been parallel transported. We expect that this non-integrability of parallel
transport characterizes the intrinsic notion of curvature, which does not depend
on the special coordinates chosen.

It is useful to say that in this sense visualization of the **first Bianchi identity** is very easy:

For visualizing **Lie bracket**: if $X$ and $Y$ are two vector fields in a neighborhood of $p$, then for sufficiently small $h$ we can

(1) follow the integral curve of $X$
through $p$ for time $h$ ;
(2) starting from that point, follow the
integral curve of $Y$ for time $h$;
(3) then follow the integral curve of $X$
backwards for time $h$ ;
(4) then follow the integral curve of $Y$
backwards for time $h$.

When $X$ and $Y$ are (linearly
independent) vector fields with $[X, Y]\ne 0$, the parallelogram is not closed.

We next look at the geometrical meaning of the **torsion tensor**. Let $p \in M$
be a point whose coordinates are $\{x^μ\}$. Let $X = \varepsilon^μ e_μ$ and $Y = \delta^μ e_μ$ be
infinitesimal vectors in $T_pM$. If these vectors are regarded as small displacements,
they define two points $q$ and $s$ near $p$, whose coordinates are $\{x^μ + ε^μ\}$ and
$\{x^μ + δ^μ\}$ respectively (following figure). If we parallel transport $X$ along the line $ps$,
we obtain a vector $sr_1$ whose component is $\varepsilon^μ − \varepsilon^{\lambda} \Gamma^{\mu}_{\nu \lambda} \delta^{\nu}$
. The displacement
vector connecting $p$ and $r_1$ is

$$pr_1 = ps + sr_1 = δ^μ + ε^μ − \Gamma^{\mu}_{\nu \lambda} \varepsilon^{\lambda} \delta^{\nu} .$$

Similarly, the parallel transport of $δ^μ$ along $pq$ yields a vector

$$pr_2 = ps + sr_2 = ε^μ + δ^μ − \Gamma^{\mu}_{\lambda \nu} \varepsilon^{\lambda} \delta^{\nu} .$$

In general, $r_1$ and $r_2$ do not agree and the difference is

$$r_2r_1=pr_2-pr_1=(\Gamma^{\mu}_{\nu \lambda}− \Gamma^{\mu}_{\lambda \nu})\varepsilon^{\lambda} \delta^{\nu}=T^{\mu}_{\lambda \nu} \varepsilon^{\lambda} \delta^{\nu} \qquad(*)$$

Thus, the torsion tensor measures the failure of the closure of the parallelogram
made up of the small displacement vectors and their parallel transports.

Now with respect to the above description it is easy to imagine the Torsion tensor in terms of the Lie bracket and connection:

$$T(u,v)=\nabla_u v −\nabla_v u−[u,v]$$

**I hope the above explanations have cleared the matter
now I will get to answering your question:**

Suppose we are navigating on the surface of the Earth. We define a
vector to be parallel transported if the angle between the vector and the latitude is
kept fixed during the navigation. [Remarks: This definition of parallel transport
is not the usual one. For example, the geodesic is not a great circle but a straight
line on Mercator’s projection.] Suppose we navigate along
a small quadrilateral $pqrs$ made up of latitudes and longitudes (following figure).

We parallel transport a vector at $p$ along $pqr$ and $psr$, separately. According
to our definition of parallel transport, two vectors at $r$ should agree, hence the
curvature tensor vanishes. To find the torsion, we parametrize the points $p$, $q$, $r$
and $s$ as in following figure.

We find the torsion by evaluating the difference between
$pr_1$ and $pr_2$ as in $(*)$. If we parallel transport the vector $pq$ along $ps$, we
obtain a vector $sr_1$, whose length is $R \sin \theta d\varphi$. However, a parallel transport
of the vector $ps$ along $pq$ yields a vector $qr_2 = qr$. Since $sr$ has a length
$R \sin(\theta − d\theta) d\varphi \simeq R \sin \theta d\varphi − R \cos \theta d\theta d\varphi$, we find that $r_1r_2$ has a length
$R \cos \theta d\theta d\varphi$. Since $r_1r_2$ is parallel to $-\frac{\partial}{\partial \varphi}$, the connection has a torsion
$T^{\varphi}_{\theta \varphi}$, see $(*)$. From $g_{\varphi \varphi} = R^2 \sin^2 \theta$, we find that $r_1r_2$ has components
$(0,−\cot \theta d\theta d\varphi)$. Since the $\varphi$-component of $r_1r_2$ is equal to $T^{\varphi}_{\theta \varphi} d\theta d\varphi$, we
obtain $T^{\varphi}_{\theta \varphi} = −\cot \theta$.