The forces acting on the object are gravity and air resistance. The gravitational force is given by \( F_g = mg \), where \( m = 10 \, \text{kg} \) and \( g = 9.81 \, \text{m/s}^2 \). The force due to air resistance is \( F_r = -bv \), where \( b = 50 \, \text{N s/m} \) and \( v \) is the velocity.
The net force \( F \) on the object is:
\[
F = mg - bv
\]
According to Newton's second law, \( F = ma \), where \( a = \frac{dv}{dt} \). Therefore, we have:
\[
m \frac{dv}{dt} = mg - bv
\]
Substituting the given values:
\[
10 \frac{dv}{dt} = 10 \times 9.81 - 50v
\]
Simplifying, we get the differential equation:
\[
\frac{dv}{dt} = 9.81 - 5v
\]
This is a first-order linear differential equation. We can solve it using separation of variables:
\[
\frac{dv}{9.81 - 5v} = dt
\]
Integrating both sides:
\[
\int \frac{1}{9.81 - 5v} \, dv = \int \, dt
\]
The left side integrates to:
\[
-\frac{1}{5} \ln |9.81 - 5v| = t + C
\]
Solving for \( v \), we exponentiate both sides:
\[
|9.81 - 5v| = e^{-5t + C}
\]
Let \( C_1 = e^C \), then:
\[
9.81 - 5v = C_1 e^{-5t}
\]
Solving for \( v \):
\[
v = \frac{9.81}{5} - \frac{C_1}{5} e^{-5t}
\]
Since the object is released from rest, \( v(0) = 0 \). Substituting into the velocity equation:
\[
0 = \frac{9.81}{5} - \frac{C_1}{5}
\]
Solving for \( C_1 \):
\[
C_1 = 9.81
\]
Thus, the velocity equation becomes:
\[
v(t) = \frac{9.81}{5} (1 - e^{-5t})
\]
The position function \( x(t) \) is the integral of the velocity function:
\[
x(t) = \int v(t) \, dt = \int \frac{9.81}{5} (1 - e^{-5t}) \, dt
\]
Integrating:
\[
x(t) = \frac{9.81}{5} \left( t + \frac{1}{5} e^{-5t} \right) + C_2
\]
Since the object starts from rest at \( x(0) = 0 \):
\[
0 = \frac{9.81}{5} \left( 0 + \frac{1}{5} \right) + C_2
\]
Solving for \( C_2 \):
\[
C_2 = -\frac{9.81}{25}
\]
Thus, the position function is:
\[
x(t) = \frac{9.81}{5} \left( t + \frac{1}{5} e^{-5t} \right) - \frac{9.81}{25}
\]
The equation of motion of the object is:
\[
\boxed{x(t) = \frac{9.81}{5} \left( t + \frac{1}{5} e^{-5t} \right) - \frac{9.81}{25}}
\]