To administer a quantitative measure up for the direction of spontaneous change, Clausius introduced the principle of entropy as a precise means of expressing the second law the thermodynamics. The Clausius kind of the second law states that spontaneous adjust for an irreversible process in an isolated system (that is, one that does no exchange warm or occupational with that is surroundings) always proceeds in the direction of boosting entropy. For example, the block the ice and the stove constitute two components of an isolated system for which total entropy increases as the ice melts.

You are watching: Which one of the following systems has the highest entropy

By the Clausius definition, if an quantity of heat Q flows right into a huge heat reservoir in ~ temperature T over absolute zero, climate the entropy boost is ΔS = Q/T. This equation properly gives one alternate an interpretation of temperature the agrees with the normal definition. Assume the there room two warm reservoirs R1 and R2 at temperatures T1 and also T2 (such together the stove and the block of ice). If an quantity of warmth Q flows from R1 to R2, climate the network entropy change for the 2 reservoirs is

which is positive listed that T1 > T2. Thus, the monitoring that heat never operation spontaneously from cold to warm is tantamount to inquiry the network entropy adjust to be hopeful for a spontaneous flow of heat. If T1 = T2, then the reservoirs are in equilibrium, no heat flows, and ΔS = 0.

The problem ΔS ≥ 0 determines the maximum feasible efficiency of heat engines—that is, solution such as gasoline or steam engines that deserve to do work-related in a cyclic fashion. Expect a warmth engine absorbs heat Q1 from R1 and exhausts warmth Q2 to R2 for each complete cycle. By conservation of energy, the job-related done every cycle is W = Q1 – Q2, and the network entropy adjust is

To do W as large as possible, Q2 should be as small as feasible relative to Q1. However, Q2 cannot be zero, due to the fact that this would certainly make ΔS an unfavorable and so violate the 2nd law. The smallest possible value of Q2 synchronizes to the problem ΔS = 0, yielding
as the basic equation limiting the performance of all heat engines. A procedure for i beg your pardon ΔS = 0 is reversible since an infinitesimal adjust would be adequate to make the warm engine operation backward as a refrigerator.

The same thinking can likewise determine the entropy readjust for the functioning substance in the warmth engine, such as a gas in a cylinder v a movable piston. If the gas absorbs one incremental amount of warm dQ indigenous a heat reservoir at temperature T and expands reversibly against the maximum feasible restraining push P, then it walk the maximum work-related dW = P dV, whereby dV is the adjust in volume. The internal power of the gas can also adjust by an lot dU as it expands. Climate by preservation of energy, dQ = dU + P dV. Since the network entropy change for the device plus reservoir is zero once maximum work-related is done and the entropy the the reservoir reduce by an quantity dSreservoir = −dQ/T, this should be counterbalanced by an entropy rise of

for the working gas so the dSsystem + dSreservoir = 0. For any type of real process, less than the maximum job-related would be done (because the friction, because that example), and so the actual lot of heat dQ′ soaked up from the warmth reservoir would be less than the maximum amount dQ. Because that example, the gas might be permitted to increase freely into a vacuum and do no occupational at all. Therefore, it can be declared that
with dQ′ = dQ in the instance of maximum work matching to a reversible process.

This equation defines Ssystem together a thermodynamic state variable, an interpretation that its worth is fully determined by the current state of the system and not by exactly how the system reached the state. Entropy is substantial property in that its magnitude counts on the amount of product in the system.

See more: Which Of The Following Weapons Helped Continue The Stalemate On Battlefields During World War I?

In one statistical interpretation the entropy, it is found that because that a very huge system in thermodynamic equilibrium, entropy S is proportional to the organic logarithm the a amount Ω representing the maximum variety of microscopic means in which the macroscopic state matching to S can be realized; that is, S = k ln Ω, in which k is the Boltzmann constant that is regarded molecular energy.

All spontaneous processes are irreversible; hence, it has actually been stated that the entropy that the cosmos is increasing: that is, more and an ext energy becomes unavailable for conversion into work. Since of this, the universe is said to be “running down.”