To solve this, we need to determine the speed required for the machine to achieve a given current as a generator, assuming it's already running at a specific speed as a motor.
Here’s a step-by-step process to find the speed at which the machine must be driven to achieve the same current as a generator:
### Given Data:
- Supply Voltage, \( V \) = 200 V
- Armature Resistance, \( R_a \) = 0.5 Ω
- Field Resistance, \( R_f \) = 200 Ω
- Current drawn from supply mains, \( I \) = 31 A (as a motor)
- Speed (as a motor), \( N_m \) = 1000 rpm (as given in the problem context)
### As a Motor:
1. **Calculate the armature current, \( I_a \):**
\[ I_a = I - \frac{V}{R_f} \]
Here, \( I \) is the total current drawn from the supply, and the field current is given by \( \frac{V}{R_f} \).
\[ I_f = \frac{V}{R_f} = \frac{200}{200} = 1 \text{ A} \]
\[ I_a = 31 - 1 = 30 \text{ A} \]
2. **Determine the back EMF, \( E \), when operating as a motor:**
\[ E = V - I_a \cdot R_a \]
\[ E = 200 - 30 \cdot 0.5 = 200 - 15 = 185 \text{ V} \]
### As a Generator:
To achieve the same current (31 A) as a generator, the back EMF \( E_g \) must be the same, but the terminal voltage \( V_g \) will now be the same as the supply voltage \( V \).
3. **Calculate the speed required for the generator operation:**
The relationship between the speed and the back EMF is given by:
\[ \frac{N_g}{N_m} = \frac{E_g}{E_m} \]
where \( E_g \) and \( E_m \) are the back EMFs as a generator and motor, respectively, and \( N_g \) and \( N_m \) are the speeds of the machine as a generator and motor, respectively.
Since the back EMF \( E_g \) is the same as \( E_m \):
\[ \frac{N_g}{N_m} = \frac{E_g}{E_m} = \frac{185}{185} = 1 \]
Therefore:
\[ N_g = N_m \]
So, the machine must be driven at the same speed as a generator to achieve the same current, which is \( 1000 \text{ rpm} \).