Step 1: One–shaft (single-spool) power balance.
Turbine and compressor sit on the same shaft. In steady state with no losses,
\[
P_t = P_c \Rightarrow \dot m\,W_t = \dot m\,W_c \Rightarrow W_t = W_c,
\]
where \(W\) is specific shaft work (per unit mass flow \(\dot m\)). The number of stages only divides the same total work among stages.
Step 2: Euler turbomachinery view (why stage count is irrelevant).
Compressor: per stage \( \Delta h_{0,\text{stg}} = U\,(V_{\theta 2}-V_{\theta 1}) \) (positive for compressor).
Turbine: per stage \( \Delta h_{0,\text{stg}} = U\,(V_{\theta 1}-V_{\theta 2}) \) (delivers work).
Total compressor work \(W_c = \sum_{i=1}^{6}\Delta h_{0,\text{stg},i}\).
Total turbine work \(W_t = \sum_{j=1}^{2}\Delta h_{0,\text{stg},j}\).
On a single spool in lossless idealization, the sums must be equal so that the shaft neither accelerates nor decelerates:
\[
\sum_{j=1}^{2}\Delta h_{0,\text{stg},j} \;=\; \sum_{i=1}^{6}\Delta h_{0,\text{stg},i}.
\]
Step 3: What multipliers (2, 3, 6) would imply.
Any \(W_t \neq W_c\) would yield net shaft power \(\dot m (W_t - W_c)\neq 0\), violating steady single-spool operation (unless unmodelled losses/drives are present, which the problem excludes).
Final Answer:
\[
\boxed{W_t = W_c}
\]
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