Question 3.8: The following readings were taken during a trial of a single...
The following readings were taken during a trial of a single-cylinder doubleacting non-condensing steam engine running at 240 r.p.m.
Cylinder diameter 250 mm
Piston rod diameter 50 mm
Stroke of the engine 350 mm
Cut-off 30% of the stroke
Length of the indicator diagram 53 mm
Area of the indicator diagram for cover end 1570 mm²
Area of the indicator diagram for crank end 1440 mm²
Spring number 0.12 bar/mm
Circumference of the brake wheel 5.25 m
Circumference of the brake rope 62.5 mm
Dead load on the brake 1900 N
Reading of the spring balance 190 N
Pressure of the steam supplied 10.5 bar
Dryness fraction of steam supplied 0.92
Find : (i) Indicated power (I.P.) ;
(ii) Brake power (B.P.) ;
(iii) Mechanical efficiency ;
(iv) Specific steam consumption on I.P. and B.P. basis ;
(v) Brake thermal efficiency.
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(i) Indicated power (I.P.) :
I.P. = \frac{10 p_{m_1} LA_{1} N}{6} + \frac{10 p_{m_2} LA_{2} N}{6} …(i)
p_{m} = \frac{Area of the indicator diagram (A ) × Spring number (S) }{Length of the indicator diagram (L)}∴ p_{m_1} = \frac{A_{1} S}{L} = \frac{1570 × 0.12 }{53} = 3.55 bar
and p_{m_2} = \frac{A_{2} S}{L} = \frac{1440 × 0.12 }{53} = 3.26 bar
A_{1} = π/4 D² = π/4 × 0.25² = 0.04908 m²
A_{2} = π/4 (D² – d²) = π/4 (0.25² – 0.05²) = 0.04712 m²
Inserting these values in eqn. (i), we get
I.P. = \frac{10 × 3.55 × 0.35 × 0.04908 × 240 }{6} + \frac{10 × 3.26 × 0.35 × 0.04712 × 240}{6}
= 24.4 + 21.5 = 45.9 kW.
(ii) Brake power (B.P.) :
B.P. = \frac{(W – S) π (D + d ) N}{60 × 10³} = \frac{(1900 – 190) × \left\lgroup 5.25 + \frac{62.5}{1000} \right\rgroup × 240 }{60 × 1000} = 36.34 kW.
(iii) Mechanical efficiency, η_{mech} : [∵ pD = 5.25 m; π d = \frac{62.5}{1000} m …Given]
η_{mech} = \frac{B.P. }{I.P.} = \frac{36.34}{45.9} = 0.7917 = 79.17%.
(iv) Specific steam consumption :
Steam consumption per hour, m_{s} = Steam consumed/revolution × r.p.m. × 60
= [(steam consumption of cover end/stroke + steam consumption of crank end/stroke) × r.p.m. × 60]
= [ \frac{π / 4 D² × L }{r} + \frac{π / 4 (D² – d²) L }{r} ] × \frac{r.p.m × 60 }{specific volume of steam}
where r = cut-off ratio.
∴ m_{s} = \frac{π}{4} . \frac{L}{r} [D² + (D² – d²)] × \frac{240 × 60}{x v_{g}}
= \frac{π}{4} × \frac{0.35}{3.33} [0.25² + (0.25² – 0.05²)] × \frac{240 × 60}{0.92 × 0.185 }
[∵ r = \frac{1}{0.3} = 3.33 and v_{g} = 0.185 m³ / kg at 10.5 bar from steam tables]
= 855.56 kg/h
Specific steam consumption on I.P. basis
\frac{855.56}{45.9} = 18.64 kg/kWh.
Specific fuel consumption on B.P. basis
\frac{855.56}{36.34} = 23.54 kg/kWh.
(v) Brake thermal efficiency:
Brake thermal efficiency,
Here h _{1} = h_{f_1} + x _{1} h_{fg_1} [At 10.5 bar, from steam tables : h_{f_1} = 772 kJ / kg, h_{fg} = 2005.9 kJ / kg]
= 772 + 0.92 × 2005.9 = 2617.4 kJ/kg
h_{f_2} = 0, since engine is non-condensing.
∴ η_{th(B)} = \frac{36.34}{\frac{855.56}{3600} × 2617.4} = 0.0584 or 5.84%.