First Law of Thermodynamics

Q: What is the difference between internal energy, heat, and work?

Internal energy ($U$) is a state function, representing the total energy contained within a system (kinetic and potential energy of molecules). Its change ($\Delta U$) depends only on the initial and final states. Heat ($q$) and work ($w$) are path functions, meaning their values depend on the specific process or path taken. Heat is energy transfer due to temperature difference, while work is energy transfer not due to temperature difference (e.g., mechanical work like expansion/compression). Both $q$ and $w$ are ways energy is transferred into or out of a system, contributing to the change in its internal energy.

Q: What is the significance of enthalpy ($\Delta H$) in relation to the First Law?

Enthalpy ($H$) is a thermodynamic property defined as $H = U + PV$. Its change, $\Delta H$, is particularly significant for processes occurring at constant pressure, which are very common in chemistry (e.g., reactions in open beakers). Under constant pressure conditions, the heat exchanged ($q_p$) is equal to the change in enthalpy ($\Delta H = q_p$). This makes enthalpy a convenient measure for tracking heat changes in isobaric processes, as it directly relates to the heat absorbed or released by the system without needing to account for PV work separately.

Updated 22 Mar 2026

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The First Law of Thermodynamics, also known as the Law of Conservation of Energy, states that energy cannot be created or destroyed in an isolated system. It can only be transformed from one form to another. In the context of a thermodynamic system, this law is expressed as the change in the internal energy of a system ( $\Delta U$ ) being equal to the heat ( $q$ ) added to the system plus the work ($…

Quick Summary

The First Law of Thermodynamics is fundamentally the law of conservation of energy applied to thermodynamic systems. It states that energy cannot be created or destroyed, only transformed. Mathematically, it's expressed as $\Delta U = q + w$ , where $\Delta U$ is the change in the system's internal energy, $q$ is the heat exchanged, and $w$ is the work done.

Internal energy ( $U$ ) is a state function, depending only on the system's current state. Heat ( $q$ ) and work ( $w$ ) are path functions, depending on the process. Key sign conventions: $q > 0$ for heat absorbed, $q < 0$ for heat released; $w > 0$ for work done on the system, $w < 0$ for work done by the system.

Different thermodynamic processes (isochoric, isobaric, isothermal, adiabatic, cyclic) lead to specific simplifications of the First Law, allowing for calculations of energy changes. Enthalpy ( $\Delta H = q_p$ ) is a crucial concept derived from the First Law for constant pressure processes.

Full explanation

The First Law of Thermodynamics is a cornerstone of physical chemistry, providing a quantitative framework for understanding energy transformations. At its heart, it is a statement of the conservation of energy, adapted for thermodynamic systems. Let's break down its components and implications.

Conceptual Foundation: Energy Conservation

Historically, the concept of energy conservation evolved from observations that energy, while changing forms, always seemed to maintain a constant total. The First Law formalizes this for thermodynamic systems.

It posits that for any process, the total energy of an isolated system remains constant. An isolated system is one that cannot exchange either matter or energy with its surroundings. For a closed system (which can exchange energy but not matter), the law states that the change in the system's internal energy ( $\Delta U$ ) is the sum of the heat ( $q$ ) transferred to or from the system and the work ( $w$ ) done on or by the system.

Key Principles and Mathematical Formulation

Internal Energy ($U$ or $E$) — This is the total energy contained within a thermodynamic system. It includes all forms of energy at the molecular level: kinetic energy (translational, rotational, vibrational motion of molecules) and potential energy (due to intermolecular forces and chemical bonds). Internal energy is a state function, meaning its value depends only on the current state of the system (temperature, pressure, volume, composition) and not on the path taken to reach that state. Therefore, for a cyclic process,

\Delta U = 0

. The absolute value of internal energy cannot be determined, but changes in internal energy (

\Delta U

) can be measured.

Heat ($q$) — Heat is the transfer of thermal energy between a system and its surroundings due to a temperature difference. Heat is a path function, meaning the amount of heat transferred depends on the specific path or process followed. By convention:

* $q > 0$ (positive) when heat is absorbed by the system from the surroundings (endothermic process). * $q < 0$ (negative) when heat is released by the system to the surroundings (exothermic process).

Work ($w$) — Work is energy transfer that is not due to a temperature difference. In chemistry, we primarily focus on pressure-volume (PV) work, which involves expansion or compression of gases. Work is also a path function. By convention (IUPAC convention, commonly used in chemistry):

* $w > 0$ (positive) when work is done on the system by the surroundings (e.g., compression). * $w < 0$ (negative) when work is done by the system on the surroundings (e.g., expansion).

The mathematical expression for work done by a system against a constant external pressure ( $P_{ext}$ ) during a volume change ( $\Delta V$ ) is:

w = -P_{ext}\Delta V

where

\Delta V = V_{final} - V_{initial}

. The negative sign ensures that if the system expands (

\Delta V > 0

), work done by the system is negative, consistent with our convention.

For reversible processes, where the external pressure is infinitesimally close to the internal pressure ( $P_{ext} \approx P_{internal}$ ), the work done is given by:

w_{rev} = -\int_{V_1}^{V_2} P_{internal} dV

For an ideal gas,

P_{internal} = \frac{nRT}{V}

, so for reversible isothermal expansion:

w_{rev} = -\int_{V_1}^{V_2} \frac{nRT}{V} dV = -nRT \ln\left(\frac{V_2}{V_1}\right)

The First Law Equation: Combining these, the First Law of Thermodynamics is stated as:

\Delta U = q + w

This equation means that any change in the internal energy of a system is accounted for by the heat exchanged with its surroundings and the work done on or by it.

Applications in Different Thermodynamic Processes

Isochoric Process (Constant Volume)

In an isochoric process, the volume of the system remains constant ( $\Delta V = 0$ ). Since $w = -P_{ext}\Delta V$ , if $\Delta V = 0$ , then $w = 0$ . Therefore, the First Law simplifies to:

\Delta U = q_v

Here,

q_v

denotes heat exchanged at constant volume. This means that all the heat supplied to the system at constant volume goes directly into increasing its internal energy.

Isobaric Process (Constant Pressure)

Most chemical reactions in open containers occur at constant atmospheric pressure. In this case, work is done due to volume changes. The First Law becomes:

\Delta U = q_p + w = q_p - P_{ext}\Delta V

Rearranging,

q_p = \Delta U + P_{ext}\Delta V

This quantity, $q_p$ , is defined as the change in enthalpy ( $\Delta H$ ). Enthalpy ( $H$ ) is defined as $H = U + PV$ . Since $U$ , $P$ , and $V$ are state functions, $H$ is also a state function. Therefore, for an isobaric process:

\Delta H = q_p

This makes enthalpy a very convenient measure for heat changes in constant pressure processes, which are common in chemistry.

Isothermal Process (Constant Temperature)

For an ideal gas, the internal energy depends only on temperature. Therefore, if the temperature is constant ( $\Delta T = 0$ ), then the change in internal energy is zero ( $\Delta U = 0$ ). The First Law then becomes:

0 = q + w \implies q = -w

This implies that any heat absorbed by the system is entirely converted into work done by the system, or vice-versa.

For a reversible isothermal expansion of an ideal gas:

w = -nRT \ln\left(\frac{V_2}{V_1}\right)

And consequently,

q = nRT \ln\left(\frac{V_2}{V_1}\right)

Adiabatic Process (No Heat Exchange)

An adiabatic process is one where no heat is exchanged between the system and its surroundings ( $q = 0$ ). This can occur if the system is perfectly insulated or if the process happens very rapidly. The First Law simplifies to:

\Delta U = w_{ad}

This means that any work done on the system increases its internal energy, and any work done by the system decreases its internal energy.

For an adiabatic expansion, the system does work, so $w_{ad} < 0$ , leading to a decrease in internal energy and thus a decrease in temperature. For an adiabatic compression, work is done on the system, $w_{ad} > 0$ , leading to an increase in internal energy and temperature.

For a reversible adiabatic process involving an ideal gas, the relationship between $P, V, T$ is given by:

PV^\gamma = \text{constant}

TV^{gamma-1} = \text{constant}

where

\gamma = C_p/C_v

is the adiabatic index.

Cyclic Process — A cyclic process is one where the system returns to its initial state after a series of changes. Since internal energy is a state function, for a cyclic process, the net change in internal energy is zero (

\Delta U_{cycle} = 0

). Therefore, from the First Law:

0 = q_{cycle} + w_{cycle} \implies q_{cycle} = -w_{cycle}

This means that the net heat absorbed by the system in a cycle is equal to the negative of the net work done by the system (i.e., the net work done on the system).

Heat Capacities ($C_v$ and $C_p$)

Heat capacity is a measure of how much heat energy is required to raise the temperature of a substance by a certain amount.

Molar Heat Capacity at Constant Volume ($C_v$) — Defined as the heat required to raise the temperature of 1 mole of a substance by

1^\circ C

(or

1 K

) at constant volume. From

\Delta U = q_v

, we can write:

q_v = n C_v \Delta T

And for infinitesimal changes,

dU = n C_v dT

. For an ideal gas,

C_v = \frac{f}{2}R

, where

f

is the degrees of freedom.

Molar Heat Capacity at Constant Pressure ($C_p$) — Defined as the heat required to raise the temperature of 1 mole of a substance by

1^\circ C

(or

1 K

) at constant pressure. From

\Delta H = q_p

, we can write:

q_p = n C_p \Delta T

And for infinitesimal changes,

dH = n C_p dT

Relation between $C_p$ and $C_v$ (Mayer's Relation)

For an ideal gas, $C_p - C_v = R$ , where $R$ is the ideal gas constant. This difference arises because at constant pressure, some of the heat supplied is used to do expansion work, in addition to increasing the internal energy.

Common Misconceptions and NEET-Specific Angle

Sign Conventions — This is the most common source of error. Always remember: heat into system is positive, work on system is positive. Conversely, heat out of system is negative, work by system is negative. The IUPAC convention (

w = -P_{ext}\Delta V

) is standard in chemistry. Physics often uses

w = PDelta V

(work done by the system), which means the First Law becomes

\Delta U = q - w_{by}

. Stick to one convention consistently.

State vs. Path Functions — Internal energy and enthalpy are state functions; heat and work are path functions. This means

\Delta U

and

\Delta H

depend only on initial and final states, while

q

and

w

depend on the process. This is critical for understanding cyclic processes and for distinguishing between

q_v

and

q_p

Ideal Gas Assumptions — Many NEET problems assume ideal gas behavior, where internal energy is solely a function of temperature. This simplifies isothermal processes (

\Delta U = 0

). Be mindful when this assumption is not explicitly stated or if the substance is not an ideal gas.

Units — Ensure consistency in units. Energy is typically in Joules (J) or kilojoules (kJ). Pressure in Pascals (Pa) or atmospheres (atm), volume in cubic meters (

m^3

) or liters (L). Remember

1\,\text{L atm} = 101.3\,\text{J}

. The gas constant

R

should be chosen appropriately (

8.314\,\text{J mol}^{-1}\text{K}^{-1}

0.0821\,\text{L atm mol}^{-1}\text{K}^{-1}

The First Law is foundational for understanding thermochemistry, chemical equilibrium, and spontaneity (though it doesn't predict spontaneity itself, that's the Second Law's domain). NEET questions often involve applying the First Law to various processes, calculating $q$ , $w$ , $\Delta U$ , or $\Delta H$ , and understanding the relationships between these quantities and heat capacities.

Key Concepts

Sign Conventions for Heat and Work

Understanding the sign conventions is paramount for correctly applying the First Law. In chemistry, we…

Work Done in Reversible Isothermal Expansion of an Ideal Gas

An isothermal process occurs at constant temperature ( $\Delta T = 0$ ). For an ideal gas, internal energy…

Relationship between

C_p

and

C_v

(Mayer's Relation)

Molar heat capacities at constant volume ( $C_v$ ) and constant pressure ( $C_p$ ) are important for relating…

Often confused with

Side-by-side differences the NEET paper likes to test.

First Law of Thermodynamics vs Internal Energy vs. Enthalpy

Aspect	First Law of Thermodynamics	Internal Energy vs. Enthalpy
Definition	Internal Energy ($U$): Total energy contained within a system (kinetic + potential energy of molecules).	Enthalpy ($H$): A thermodynamic potential defined as $H = U + PV$ (Internal energy + Pressure-Volume work).
Nature	State function. Its change ($\Delta U$) depends only on initial and final states.	State function. Its change ($\Delta H$) depends only on initial and final states.
Measurement	Change in internal energy ($\Delta U$) is equal to heat exchanged at constant volume ($q_v$). $\Delta U = q_v$.	Change in enthalpy ($\Delta H$) is equal to heat exchanged at constant pressure ($q_p$). $\Delta H = q_p$.
Relevance	Most relevant for processes occurring at constant volume (isochoric processes), or when considering total energy changes irrespective of pressure-volume work.	Most relevant for processes occurring at constant pressure (isobaric processes), which are common in chemical reactions conducted in open vessels.
Relation to First Law	Directly appears in the First Law: $\Delta U = q + w$.	Derived from the First Law under constant pressure conditions: $\Delta H = \Delta U + PDelta V = (q_p + w) + PDelta V = q_p - PDelta V + PDelta V = q_p$.

While both internal energy and enthalpy are state functions representing energy within a system, they differ in their practical application and definition. Internal energy ( $U$ ) represents the total microscopic energy, and its change ( $\Delta U$ ) directly equals heat exchanged at constant volume ( $q_v$ ).

Enthalpy ( $H$ ), defined as $U+PV$ , is particularly useful for constant pressure processes, where its change ( $\Delta H$ ) directly corresponds to the heat exchanged ( $q_p$ ). This distinction is crucial for correctly analyzing energy changes in different experimental conditions.

Why it is tested: For NEET, understanding the distinction between $\Delta U$ and $\Delta H$ is critical. Many problems involve calculating heat changes for reactions, and knowing when to use $\Delta U$ (constant volume) versus $\Delta H$ (constant pressure) is a common test of conceptual clarity. Questions often involve converting between $\Delta U$ and $\Delta H$ using the relation $\Delta H = \Delta U + \Delta n_g RT$ for gaseous reactions.

Questions students ask

6 answered on this topic.

What is the primary statement of the First Law of Thermodynamics?

The primary statement of the First Law of Thermodynamics is the principle of conservation of energy. It asserts that energy can neither be created nor destroyed, but can only be transformed from one form to another. For a thermodynamic system, this translates to the mathematical expression $\Delta U = q + w$ , where $\Delta U$ is the change in internal energy, $q$ is the heat exchanged, and $w$ is the work done. This means the total energy of an isolated system remains constant.

What is the difference between internal energy, heat, and work?

Internal energy ( $U$ ) is a state function, representing the total energy contained within a system (kinetic and potential energy of molecules). Its change ( $\Delta U$ ) depends only on the initial and final states.

Heat ( $q$ ) and work ( $w$ ) are path functions, meaning their values depend on the specific process or path taken. Heat is energy transfer due to temperature difference, while work is energy transfer not due to temperature difference (e.

g., mechanical work like expansion/compression). Both $q$ and $w$ are ways energy is transferred into or out of a system, contributing to the change in its internal energy.

Why is internal energy considered a state function, but heat and work are not?

Internal energy is a state function because its value is determined solely by the current state variables of the system (like temperature, pressure, volume). Regardless of how the system reached that state, its internal energy will be the same.

Heat and work, however, are path functions because the amount of heat exchanged or work done depends entirely on the specific process or 'path' followed between the initial and final states. Different paths between the same two states will generally involve different amounts of heat and work, even if the change in internal energy is the same.

What are the sign conventions for heat and work in the First Law equation?

The IUPAC sign conventions, commonly used in chemistry, are crucial for applying the First Law correctly. Heat ( $q$ ) is positive when absorbed by the system (endothermic) and negative when released by the system (exothermic). Work ( $w$ ) is positive when done on the system by the surroundings (e.g., compression) and negative when done by the system on the surroundings (e.g., expansion). This convention ensures consistency in the $\Delta U = q + w$ equation.

How does the First Law apply to an adiabatic process?

An adiabatic process is characterized by no heat exchange between the system and its surroundings, meaning $q=0$ . In this scenario, the First Law simplifies to $\Delta U = w_{ad}$ . This implies that any change in the internal energy of the system is solely due to the work done on or by the system.

If the system does work (expansion), its internal energy decreases, leading to a drop in temperature. If work is done on the system (compression), its internal energy increases, causing a rise in temperature.

What is the significance of enthalpy ($\Delta H$) in relation to the First Law?

Enthalpy ( $H$ ) is a thermodynamic property defined as $H = U + PV$ . Its change, $\Delta H$ , is particularly significant for processes occurring at constant pressure, which are very common in chemistry (e.

g., reactions in open beakers). Under constant pressure conditions, the heat exchanged ( $q_p$ ) is equal to the change in enthalpy ( $\Delta H = q_p$ ). This makes enthalpy a convenient measure for tracking heat changes in isobaric processes, as it directly relates to the heat absorbed or released by the system without needing to account for PV work separately.

Revise in 30 seconds

First Law —

\Delta U = q + w

(Conservation of Energy)

Internal Energy ($U$) — State function. For ideal gas,

U = f(T)

only.

\Delta U = nC_v\Delta T

Heat ($q$) — Path function.

+q

(absorbed),

-q

(released).

Work ($w$) — Path function.

+w

(on system),

-w

(by system).

PV Work —

w = -P_{ext}\Delta V

Reversible Isothermal Work (Ideal Gas) —

w = -nRT \ln(V_2/V_1) = -nRT \ln(P_1/P_2)

Isochoric Process ($\Delta V = 0$) —

w = 0 \implies \Delta U = q_v

Isobaric Process ($P = \text{constant}$) —

w = -P\Delta V \implies \Delta H = q_p

. Enthalpy

H = U + PV

Isothermal Process ($\Delta T = 0$) — For ideal gas,

\Delta U = 0 \implies q = -w

Adiabatic Process ($q = 0$) —

\Delta U = w_{ad}

Cyclic Process —

\Delta U = 0 \implies q_{cycle} = -w_{cycle}

Mayer's Relation (Ideal Gas) —

C_p - C_v = R

Conversion —

1\,\text{L atm} = 101.3\,\text{J}

To remember the First Law and its signs: 'Q-W-U'

Queer Work Understood:

\Delta U = q + w

Queer (Heat): Quickly Increases (positive for absorbed), Out (negative for released).

Work: When On (positive for on system), By (negative for by system).

For processes: 'I-A-I-A-C' (Isothermal, Adiabatic, Isochoric, Isobaric, Cyclic)

Isothermal: Temperature Constant (

\Delta T=0 \implies \Delta U=0 \implies q=-w

for ideal gas).

Adiabatic: Quiet (No heat,

q=0 \implies \Delta U=w

Isochoric: Volume Constant (

\Delta V=0 \implies w=0 \implies \Delta U=q_v

Isobaric: Pressure Constant (

\Delta H=q_p

Cyclic: U-turn (Back to start,

\Delta U=0 \implies q=-w