Answer:
To solve this problem, we can use the principles of static equilibrium. In this position, the person is not accelerating vertically, so the sum of forces in the vertical direction is zero, and the sum of torques (moments) about any point is zero.
**(a) Normal Force:**
Let's consider the entire body as a system. The person's weight (\(W_{\text{total}} = 750 \, \text{N}\)) acts downward from the center of mass (C) of the entire body.
\[ W_{\text{total}} = W_{\text{legs}} + W_{\text{trunk}} \]
1. **Weight of Legs (\(W_{\text{legs}}\)):**
\[ W_{\text{legs}} = 277 \, \text{N} \]
The center of mass of the legs (\(C_{\text{legs}}\)) is 41 cm from the hip.
2. **Weight of Trunk (\(W_{\text{trunk}}\)):**
\[ W_{\text{trunk}} = 473 \, \text{N} \]
The center of gravity of the trunk (\(C_{\text{trunk}}\)) is 65 cm from the hip.
Now, we can find the normal force (\(N\)) on each foot and each hand.
\[ N = \frac{W_{\text{legs}}}{2} + \frac{W_{\text{trunk}}}{2} \]
Substitute the given values and solve for \(N\).
**(b) Friction Force:**
In the downward-facing dog position, the friction force (\(f\)) prevents slipping. We'll consider the friction on the feet and the hands separately.
1. **Friction on Feet (\(f_{\text{feet}}\)):**
\[ f_{\text{feet}} = \mu_{\text{feet}} \cdot N_{\text{feet}} \]
2. **Friction on Hands (\(f_{\text{hands}}\)):**
\[ f_{\text{hands}} = \mu_{\text{hands}} \cdot N_{\text{hands}} \]
The coefficient of friction (\(\mu\)) is not provided, so it's a symbolic variable in the equations. You would need the specific value to find the actual friction force.
This approach considers the entire body as a system and then breaks down the forces for each part.